TEC =
LINE
INFORMÁTICA
PROF=
. WILSON
DAMIÃO
ELETRÔNICA =
BÁSICA
U=
m bom
curso de hardware começa com eletricidade básica, a mesma que
é estudada no segundo grau. São aprendidas noçõ=
es
sobre tensão, corrente, resistência, baterias. De posse dessas
noções, são estudados os semicondutores, como transist=
ores
e diodos. Outros componentes eletrônicos são também
estudados, como os capacitores e bobinas. O aluno aprende a construir e
consertar fontes de alimentação, amplificadores, rádios
transmissores e receptores. Finalmente chega a vez dos circuitos integrados
(chips), entrando assim na etapa de eletrônica digital. Aprend=
emos
a construir cuircuitos digitais simples, como
contadores, displays, somadores, multiplexadores, decodificadores, etc. Um
técnico formado assim está apto a consertar equipamentos digi=
tais
em geral, e não apenas computadores.
P=
ara
consertar PCs, tais
conhecimentos não são suficientes, e também não=
podem
ser considerados indispensáveis. Mais importante é ter uma boa
idéia sobre o funcionamento do computador, saber identificar se um
módulo está ou não funcionando, conhecer detalhes sobr=
e o
sistema operacional, aprender a resolver conflitos de hardware. Por isso
é possível trabalhar com hardware de PCs sem nunca ter feito um curso de eletrô=
;nica,
sem ter noções sobre transistores, resistores e outros
componentes.
A=
creditamos
que consertar um computador ou trabalhar com o seu hardware, montando ou
fazendo expansões, sem ter noções de eletrônica
é como dirigir um automóvel sem ter noções
básicas sobre mecânica. O ideal é ter o conhecimento
básico completo, mas o estudo de eletrônica básica pode=
ser
muito demorado. Para cobrir todos os seus assuntos seria preciso um livro
tão extenso quanto este. Já que se torna imprtaticável
para quem não dispõe de tempo, apresentamos neste capí=
tulo
um curso intensivo de eletrônica. Concentraremos nossa
atenção em apresentar os componentes eletrônicos usados=
nas
placas do computador e dar noções básicas sobre soldag=
em e
o uso do multímetro, aparelho que pode ajudar bastante um
técnico. Mostramos o funcionamento dos chips, circuitos digitais e
alguns outros circuitos importantes encontrados nos PCs. Essas noções serão
necessárias para que você acompanhe o restante do livro.
No&cced=
il;ões
sobre soldagem
A=
soldagem
é uma prática bastante conhecida dos técnicos, mas
não é preciso ser um técnico para saber soldar.
É fácil, e você poderá ir be=
m mais
longe nas suas atividades de hardware. A primeira coisa a fazer &eac=
ute;
ir a uma loja de material eletrônico e adquirir o seguinte:
- Ferro de soldar de 24 ou 30 watts <=
/li>
- Sugador de solda
- Rolo de solda para eletrônica (a mais
fina)
- Placa universal de circuito impresso
- Resistores (qualquer valor) de 1/4 ou 1/8 =
W
- Capacitores de poliéster, qualquer =
valor
- Transistores BC548 ou similar
- Alicate de corte e alicate de bico =
- Garra jacaré tamanho pequeno=
Os
valores dos transistores, capacitores e resistores acima não s&atild=
e;o
importantes. Pode comprar os mais baratos que encontrar. Serão usados
apenas no treinamento de soldagem e dessoldagem=
. A
figura 1 mostra alguns dos componentes e ferramentas descritos acima.
|
|
Figura
3.1
Material
para treinamento de soldagem.
a)
Transistor
b) Capacitores
c) Resistores
d) Garras jacaré
e) Placa universal
f) Solda
g) Ferro de soldar
h) Sugador de solda
|
Soldage=
m
L=
igue o
ferro de soldar e espere cerca de 1 minuto até que esteja na tempera=
tura
ideal. Para verificar se a temperatura está boa, encoste a ponta do =
fio
de solda na ponta do ferro de soldar. A solda deverá derreter com
facilidade. Vamos começar soldando um resistor. Coloque o resistor
encaixado em dois furos da placa universal de circuito impresso. Feito
isso, aqueça com a ponta do ferro de soldar o terminal do resis=
tor
e o cobre da placa de circuito impresso (figura 2). Ambos devem ser aqueci&=
shy;dos
para que a solda possa derreter facilmente. Encoste agora a ponta do fio de
solda na junção aquecida entre a placa e o terminal do resist=
or.
Mantenha o tempo todo a ponta do ferro de soldar também encostando nessa junção. A solda dever&a=
acute;
derreter uniformemente. Afaste o fio de solda e depois o ferro de soldar. D=
entro
de aproximadamente dois ou três segundos a solda estará
sólida. Use o alicate de corte para retirar o excesso do termin=
al
do resistor que sobrou.
|
|
Figura
3.2
Soldagem
de um resistor.
|
T=
reine a
soldagem com os resistores e com os capacitores. Não exagere na quan=
tidade
de solda. Deve ficar uma quantidade semelhante à que você obse=
rva
nas placas do computador. Não sopre a solda para que esfrie. Es=
pere
três segundos e a solda esfriará sozinha. Não mova o
componente enquanto a solda ainda não estiver solidificada.
Na
soldagem de transistores você deverá tomar um pouco mais de
cuidado, pois são muito sensíveis ao calor. Se o ferro de sol=
dar
ficar encostado em seus terminais por mais de cinco segundos poderá
danificá-lo. Para reduzir o calor no transistor (o objetivo é
esquentar apenas a parte que será soldada) prenda uma garra
jacaré no terminal do transistor que estiver sendo soldado, do outro
lado da placa, como indicado na figura 3.
|
|
Figura
3.3
Soldagem
de um transistor.
|
Q=
uando
for realizar uma soldagem "pra valer", lembre-se que a maioria dos componentes possuem polaridade, ou =
seja,
uma posição correta para encaixe. Normalmente existe alg=
uma
indicação da posição correta na placa de circui=
to
impresso. Se não existir tal indicação anote a
posição correta antes de retirar o componente defeituoso,
para que o novo componente seja posicionado com a polaridade correta. Alguns
componentes simplesmente não funcionam se forem soldados de forma
invertida (Ex.: diodos, LEDs).
Outros podem ser permanentemente danificados pela inversão
(transistores, capacitores eletrolíticos, chips).
Dessoldagem
A=
dessoldagem é um pouco mais fácil no ca=
so de
resistores, capacitores, diodos e transistores. No caso de chips é m=
ais
difícil devido ao grande número de terminais. O sugador de so=
lda
possui um êmbolo de pressão que remove a solda derretida dos
circuitos. A figura 4 mostra como operá-lo. Primeiro pressione o seu
êmbolo, depois aproxime o seu bico da solda derretida e pressione o
botão para que o bico sugue a solda. O sugador puxará a solda
derretida para o seu interior. Aperte novamente o êmbolo para que pos=
sa
expelir a solda retirada, já no estado sólido. =
|
|
Figura
3.4
Usando
o sugador de solda.
|
A=
rme o sugador
de solda pressionando o êmbolo para baixo e deixando-o pronto para su=
gar.
Encoste o ferro de solda quente no ponto de solda que você quer re&sh=
y;mover.
A solda deverá derreter. Se estiver difícil de derreter, colo=
que
um pingo de solda nova na ponta do ferro de soldar para facilitar a
condução térmica, derretendo mais facilmente a so=
lda
da junção a ser desfeita. Sem tirar a ponta do ferro de solda=
r,
encoste o bico do sugador (figura 5) na solda derretida e dispare. Se o com=
ponente
não ficar totalmente solto, encaixe uma chave de fenda e puxe-o leve=
mente,
usando a chave como alavanca. Encoste agora o ferro de soldar novamente no
terminal e o componente sairá com facilidade.
|
|
Figura
3.5
Dessoldando componentes.
|
&=
Eacute;
desaconselhável a dessoldagem de chips p=
or
principiantes. Além de ser uma operação muito mais
difícil, os chips são extremamente sensíveis à
temperatura. Sua soldagem e dessoldagem deve ser feita apenas em laboratórios especiali=
zados,
equipados com uma estação de soldagem profissional.
Usando =
um
multímetro digital
Um
multímetro digital pode ajudar bastante nas atividades de hardw=
are,
principalmente em manutenção. Com ele você=
; pode
checar as tensões da fonte de alimentação e da rede
elétrica, checar o estado da bateria da placa de CPU, verificar se o=
drive de CD-ROM está reproduzindo CDs de
áudio, acompanhar sinais sonoros, verificar cabos e várias ou=
tras
aplicações. Seu custo é menor do que você pensa.=
Com
cerca de 30 reais você compra um modelo si=
mples,
e com cerca de 100 reais é possível comprar um modelo mais
sofisticado.
|
|
Figura
3.6
Multímetro
digital.
|
Um
multímetro possui duas pontas de prova, uma vermelha e uma preta. A
preta deve ser conectada no ponto do multímetro indicado com GND ou =
COM
(este é o chamado “terra”). A ponta de prova vermelha po=
de
ser ligada em outras entradas, mas para a maioria das medidas realizad=
as,
a ligação é feita no ponto indicado com V-=
W-mA.
U=
ma chave
rotativa é usada para selecionar o tipo de medida elétrica a =
ser
feita: V para voltagem, W para resistência e =
mA para corrente. Uma chave é usada para=
a
medição de voltagens em AC (corrente alternada) ou DC (corren=
te
contínua). Por exemplo, para medir as tensões da fonte de
alimentação, ou a tensão da bateria, usamos a chave em DC. Para medir a
tensão presente na saída de áudio de um drive de CD-ROM ao tocar um CD musical (um tipo de co=
rrente
alteranada), usamos =
a escala
AC. Para medir as tensões da rede elétrica, também
utilizamos a escala AC.
A=
lguns
multímetros possuem um único conjunto de escalas para voltage=
m, e
uma chave adicional para escolher entre AC e DC. Outros modelos, como o da
figura 6, não possuem esta chave AC/DC, e sim grupos independentes de
escalas para voltagens e correntes em AC e DC. A maioria dos
multímetros não mede corrente alternada (ACA), apenas
corrente contínua (DCA), tensão alternada (ACV) e tensã=
;o
contínua (DCV).
P=
ara cada
grandeza elétrica existem várias escalas. Por exemplo, entre =
as
várias posições da chave rotativa, podem existir algum=
as
específicas para as seguintes faixas de voltagem: 200 mV, 2 V, 20 V, 200 V e 200=
0 V.
Se
você pretende medir a tensão da bateria da placa de CPU (em to=
rno
de 3 volts), não use a escala de 2V, pois
tensões acima de 2V serão indicadas como 1,9999 V. Escolha
então a escala de 20V, pois terá condições de f=
azer
a medida esperada. Da mesma forma, para medir a tensão de uma rede
elétrica de 220 volts (use AC, pois trata-se de
tensão alternada), não escolha a escala de 200 volts, pois a
máxima tensão medida será de 199,99 volts. Escolha
então a escala de 2.000 volts ou outra para tensões elevadas.
Como regra geral, sempre que a leitura indicada tem valor máximo ou
outra indicação que esteja fora da escala, devemos utilizar u=
ma
escala maior. Quando não temos idéia aproximada da tens&atild=
e;o
que vamos medir, devemos começar com a escala de maior valor poss&ia=
cute;vel,
pois se medirmos uma tensão muito elevada usando uma escala baixa,
podemos danificar o aparelho.
|
|
Figura
3.7
Medição
de voltagem.
|
P=
ara medir
a tensão entre dois pontos, selecione a escala e encoste as pontas de
prova nos terminais nos quais a tensão de=
ve ser
medida (figura 7). Muitas vezes queremos fazer medidas de tensão
relativas ao terra (o terminal “negativo&#=
8221;
da fonte de alimentação). Você pode então fixar a
ponta de prova preta em um ponto ligado ao terra=
(por
exemplo, os fios pretos do conector de alimentação da placa de
CPU) e usar a outra ponta de prova para medir a tensão no ponto
desejado.
A
medição de resistência também possui vári=
as
escalas, e você deve escolher uma escala que comporte a medida a ser
realizada. Se você não tem idéia da escala a ser usada,
escolha a maior delas. Por exemplo, se medir um resistor de cerca de 150 oh=
ms
em uma escala de 20.000, será apresentado o valor 150. Se quiser mai=
or
precisão pode usar escalas menores. Por exemplo, na escala de 2000 o=
hms,
o valor medido poderá ser 150,3 e na escala de 200 poderá
ser 150,37.
N=
ote que
não podemos medir o valor de um resistor quando ele está em um
circuito. O valor medido será influenciado pelos demais componentes =
do
circuito ligados ao resistor. A medida correta é feita quando o resi=
stor
está desacoplado do circuito, como mostr=
a a
figura 8.
|
|
Figura
3.8
Medindo
o valor de um resistor.
Cuidado: para resistores c=
om
valores acima de 10k ohms, é recomendável não tocar =
as
mãos nas pontas de prova do multímetro, pois a
resistência do corpo humano provocará erro na medida.=
|
P=
odemos
usar o multímetro na escala de resistência para verificar se um
cabo está partido ou se um fusível está queimado. Quan=
do
um fio ou fusível está em perfeitas condições, =
sua
resistência é bem baixa, em geral inferior a 1 ohm. Colocamos
então o multímetro na escala mais baixa de resistência e
fazemos a medida. Quando o cabo está part=
ido ou
o fusível está queimado, a resistência é muito a=
lta,
e quando está bom é baixa. Note que para fazer essas medidas
é preciso que o circuito esteja desligado.
M=
uitos
multímetros possuem ao lado da escala de resistência, uma esca=
la
que emite um beep através de um pequeno =
alto
falante em caso de resistência baixa. Desta forma é
possível medir as ligações sem ter que olhar para o
display do multímetro. Prestamos atenção apenas nas
conexões que estão sendo medidas e no som emitido. Na
gíria de eletrônica isto é chamado de “bipar o circuito”.
A
medição de corrente é feita de forma um pouco diferent=
e.
Precisamos escolher a escala mais adequada, assim como nas medidas de
tensão e resistência, mas as pontas de prova devem ser
colocadas em série com o fio por onde passa a corrente a ser medida.=
Em
muitos casos é preciso cortar e desencapar o fio para fazer a
medida, e soldar e isolar o corte posteriormente. Como é uma
operação trabalhosa, devemos fazê-la apenas em caso de
necessidade.
|
|
Figura
3.9
Os
multímetros possuem entradas adicionais para medir altas
tensões e altas correntes.
O deste
exemplo possui uma entrada para medir volts, ohms e Hertz (este mede
também freqüência), uma outra entrada para medir miliampères e outra para correntes de at&eac=
ute;
10 ampères. Alguns multímetros =
podem
ainda medir transistores para verificar se estão bons ou queimados=
.
|
T=
ome
cuidado, pois a ponta de prova vermelha poderá precisar ser colocada=
em
outras entradas, dependendo da grandeza a ser medida. Em geral os
multímetros possuem entradas adicionais para medir altas voltagens e=
altas
correntes. Certos modelos possuem uma entrada independente para
medição de corrente (figura 9).
Alguns
componentes eletrônicos
V=
amos
agora apresentar alguns componentes eletrônicos e suas propriedades
elétricas. Não serão
conhecimentos suficientes para você projetar e consertar circuitos
complexos, como monitores e fontes, mas darão uma boa
noção sobre o que você irá encontrar.
Bateria=
e
fonte de alimentação
N=
enhum
circuito elétrico ou eletrônico pode funcionar sem um gerador =
de
corrente elétrica. Os geradores nada mais são que baterias,
pilhas ou fontes de alimentação. Possuem dois terminais, send=
o um
positivo e um negativo. O terminal positivo é aquele por onde
“sai” a corrente, e o negativo é aquele por onde
“entra” a corrente.
|
|
Figura
3.10
Baterias
e o seu símbolo.
|
A=
figura
11 mostra o diagrama de um circuito de uma lanterna, no qual temos uma
lâmpada alimentada por uma bateria. A corrente elétrica sai do
terminal positivo da bateria e trafega através do fio. Chegando &agr=
ave;
lâmpada, a energia elétrica é transformada em energia
luminosa e calor. Depois de atravessar a lâmpada, a corrente retorna
à bateria através do seu terminal negativo. Uma bateria &eacu=
te;
na verdade um dispositivo que empurra a corrente elétrica atrav&eacu=
te;s
dos fios ligados aos seus terminais.
|
|
Figura
3.11
Esquema
elétrico de uma lanterna. A letra “i” é usada p=
ara
designar a corrente elétrica.
|
T=
oda
bateria tem uma voltagem especificada. As pilhas, por exemplo, têm 1,5
volts. Também são bastante populares as baterias de 9 volts. =
Hoje
em dia encontramos vários tipos de bateria com diversas voltagens,
inclusive recarregáveis. É o caso das baterias de telefones
celulares.
Em
operação normal, uma bateria deve ter circuitos ligados aos s=
eus
terminais. A corrente elétrica faz com que esses circuitos funcionem.
Por exemplo, se o circuito consistir em uma simples lâmpada, o
funcionamento é caracterizado pelo acendimento desta lâmpada.
É o que chamamos de circuito fechado. Uma bateria pode
também estar desligada. Neste caso, existe tensão entre seus
terminais, porém não existe corrente. A bateria não
está portanto fornecendo energia
elétrica ao circuito. É o que ocorre quando temos uma bateria
isolada, fora do circuito, ou então quando o interruptor (ou chave)
está desligado. Chamamos esta situação de circuito
aberto.
U=
ma situação
anormal é o chamado curto-circuito. Temos um fio ligando diretamente=
os
dois terminais da bateria. A corrente atravessa o fio, porém como
não existe circuito para alimentar, esta corrente tem enorme facilid=
ade
para trafegar. Isto faz a corrente atingir um valor altíssimo, e ger=
ando
muito aquecimento. O fio pode até mesmo derreter e pegar fogo, a bat=
eria
pode esquentar até ser danificada. Para proteger equipamentos de curto-circuitos acidentais, usamos fusíveis. Se
você ligar os dois terminais de uma pilha através de um fio, o
curto circuito não será muito perigoso, mas se ligar os dois
terminais de uma tomada elétrica, pode até provocar um
incêndio.
|
|
Figura
3.12
Circuito
aberto e curto circuito. Em um circuito aberto, a corrente é sempre
zero. No curto circuito, a corrente pode ser, do ponto de vista
matemático, infinita. Na prática isto não ocorre, ma=
s a
corrente tende a apresentar um valor bastante elevado e perigoso.<=
/p>
|
A=
figura
12 mostra as características de uma bateria em aberto e outra em curto. Na bateri=
a em
aberto, a tensão entre os terminais é igual à
tensão da bateria (vamos chamá-la de V0), e a corr=
ente
vale 0. Quando a bateria está em curto, a tensão entre os
terminais vale 0, e a corrente assume um valor elevadíssimo. Usando
componentes teóricos, a corrente tenderia a ser infinita. Na
prática isto não ocorre, mas atinge um valor alto, dependendo=
das
características da bateria.
A=
fonte
de alimentação é um circuito que tem a mesma
função de uma bateria. Ela recebe a tensão da rede
elétrica e realiza várias operações:
redução, retificação, filtragem e
regulação. O resultado é uma tensão
contínua, semelhante à fornecida por baterias. Mais adiante n=
este
capítulo mostraremos como uma fonte de alimentação rea=
liza
este processo.
Resisto=
r
E=
ste
é o mais básico componente eletrônico. Muitos o chamam
erradamente de resistência. Seu nome certo é resistor, =
e a
resistência é a sua característica elétrica. Ain=
da
assim o público leigo usa termos como “a resistência do
chuveiro elétrico”, “resistência do aquecedor̶=
1;,
“resistência do ferro de passar”, “resistênci=
a da
torradeira”. Esses dispositivos são
resistores formados por fios metálicos com resistência baixa. =
Ao
serem ligados em uma tensão elétrica, são atravessados=
por
uma elevada corrente, resultando em grande dissipação de calo=
r.
Note que nas resistências desses aparelhos, o objetivo principal &eac=
ute;
a geração de calor. Já nos circuitos eletrônicos,
suas funções são outras, e não gerar calor. Os
resistores usados nesses circuitos devem ter valores tais que possam fazer o
seu trabalho com a menor geração de calor possível. &n=
bsp;
|
|
Figura
3.13
Resistores
e o seu símbolo.
|
Os
resistores usados nos circuitos eletrônicos são de vári=
os
tipos e tamanhos. Seus dois parâmetros elétricos importantes <=
span
class=3DGramE>são a resistência e a potência.
Resistores que irão dissipar muita potência elétrica
são de maior tamanho, e vice-versa. Os mostrados na figura 13 s&atil=
de;o
de 1/8 W. Existem resistores de 1/4W, 1/2W, 1W, 2W, 5W, 10W e valores ainda
mais elevados. A figura 13 mostra também o símbolo usado para
representar o resistor quando desenhamos um diagrama elétrico.
T=
odo resitor tem um valor, que é a chamada resis=
tência.
A unidade usada para medir a resistência é o ohm, cujo
símbolo é W. A voltagem gerada por uma
bateria tem seu valor dado em volts, cujo símbolo é V.=
A
unidade usada para medir a corrente elétrica é o ampère, cujo símbolo é A.=
OBS: Durante a editoração do livro ocorreram neste
capítulo (3) algumas trocas da letra grega ômega (=
W), pela letra W, devido a um erro de editoraç&atild=
e;o.
Nesta versão on-line motramos em vermelh=
o as
correções que se aplicam.
E=
xiste
uma relação direta entre a tensão aplicada sobre um
resistor, a corrente que o atravessa e o valor da sua resistência. Es=
ta
relação é a chamada lei de Ohm. Ela diz que se =
um resitor de valor R é ligado a uma tensã=
o V, sua corrente i é dada por:
i =3D
V/R
é
o mesmo que escrever:
V=
=3D R.i
P=
or
exemplo, na figura 14 ligamos uma bateria de 12 V em um resistor de 6=
W. De acordo com a lei de ohm=
, a
corrente que atravessará o resistor será de:
i =3D
12V ¸ 6=
W =3D 2A
|
|
Figura
3.14
Relação
entre corrente, tensão e resistência.
|
E=
ventualmente
podemos encontrar em circuitos, resistores ligados uns aos outros. Dizemos =
que
os resistores estão associados. As duas principais formas de
associação de resistores são as do tipo séri=
e
e parelela. Ambas são mostradas na
figura 15. Quando dois resistores estão em série, a
resistência total é igual à soma das resistências=
de
cada resistor. Portanto é calculada pela fórmula:
R=
t
=3D R1 + R2 + R3 + ... + Rn
Q=
uando os
resistores estão associados em paralelo, a fórmula da
resistência equivalente é:
1=
/Rt
=3D 1/R1 + 1/R2 + 1/R3 + ... + 1/Rn
O=
u seja,
o inverso da resistência equivalente é igual à soma dos=
inversos
das resistências individuais.
|
|
Figura
3.15
Associações
de resistores.
|
O=
utra
grandeza elétrica importante é a potência. Ela
representa a quantidade de energia elétrica que está sendo
consumida por um resistor quando é percorrido por uma corrente, e
é medida em watts, cujo símbolo é W. Quando um
resistor R é ligado a uma tensão V e percorrido por uma corrente i, a potência elétrica P pod=
e ser
calculada de várias formas equivalentes:
P=
=3D V.i
P=
=3D R.i2
P=
=3D V2/R
P=
or
exemplo, um resistor de 6W ligado a uma fonte de 12 V d=
issipa
uma potência de:
P=
=3D 122
/ 6 =3D 144/6 =3D 24 watts
&=
Eacute;
quantidade de calor suficiente para causar uma boa queimadura ao tocarmos n=
este
resistor. Ao contrário do que ocorre na física do segundo gra=
u,
não usamos na prática resistores de valores tão baixos,
nem operamos com correntes tão elevadas, pelo menos na maioria dos
casos. Os resitores em usados em eletrôni=
ca
apresentam em geral resistências da ordem de milhares de ohms, e as
correntes elétricas normalmente assumem valores da ordem de
milésimos de Ampères. Por isso us=
amos
em eletrônica as unidades kW e mA para medir resistência e corrente. As
fórmulas continuam válidas, apenas utilizamos medidas diferen=
tes
para resistência e corrente. Por exemplo, um resistor de 6 k=
W
ligado em uma fonte de=
12 V
será percorrido por uma corrente de:
i =3D
V/R =3D 12 / 6 =3D 2 mA.
A
potência elétrica neste caso é dada em miliwatts
(milésimos de Watt), cujo símbolo é mW:
P=
=3D V2/R
=3D 122 / 6 =3D 24 mW.
E=
sta
potência é tão pequena que praticamente não
percebemos que o resistor está quente. Gerar calor não &eacut=
e; o
objetivo dos circuitos eletrônicos, portanto devemos utilizar resisto=
res
com os maiores valores possíveis, desde que em condiçõ=
es
de manter em funcionamento correto os demais componentes.
Capacit=
or
O
capacitor é um componente eletrônico capaz de armazenar e forn=
ecer
cargas elétricas. Ele é formado por duas placas paralelas,
separadas por um material isolante, chamado dielétrico. Quand=
o o
ligamos a uma tensão fixa, momentaneamente passa por ele uma pequena
corrente, até que suas placas paralelas fiquem carregadas. Uma fica =
com
cargas negativas (elétrons) e outra com cargas positivas (falta de
elétrons).
|
|
Figura
3.16
Capacitores
e seu símbolo.
|
E=
xistem
vários tipos de capacitores, e as principais diferenças
estão nos valores e nas tensões elétricas suportadas. =
Um
capacitor que vai ser ligado a uma tensão de 50 volts deve ser maior=
que
outro de mesmo valor mas que vai ser ligado a uma
tensão de apenas 10 volts. Um capacitor sofre ruptura do
dielétrico quando é ligado a uma tensão mais elevada q=
ue a
especificada. Em outras palavras, ele explode!
O=
valor
de um capacitor é chamado de capacitância. A grandeza u=
sada
para medi-la é o faraday, cujo
símbolo é F. O faraday é u=
ma
unidade muito grande para medir os capacitores da vida real. Um capacitor d=
e 1F seria imenso. Encontr=
amos na
prática capacitores medindo algo da ordem de milésimos ou
milionésimos do faraday. Por isso &eacut=
e;
mais comum usar o microfaraday (=
mF) para medir os capacitores=
. Um
capacitor de 4700 mF, por exemplo, é considerado de tamanho=
relativamente
grande para um circuito eletrônico. Ainda assim existem os chamados <=
span
class=3DSpellE>supercapacitores, que possuem capacitânc=
ias da
ordem de alguns faradays, entretanto não
são empregados em circuitos eletrônicos devido ao seu grande
tamanho.
Os
capacitores têm várias aplicações nos circuitos
eletrônicos. Um das principais é a filtragem. Eles podem
acumular uma razoável quantidade de cargas quando estão ligad=
os a
uma tensão. Quando esta tensão é desligada, o capacitor
é capaz de continuar fornecendo esta mesma tensão durante um
pequeno período de tempo, funcionando portanto
como uma espécie de bateria de curta duração. <=
/span>
|
|
Figura
3.17
Capacitores
de desacoplamento, um ao lado de cada chip.
|
Em
qualquer placa de circuito, encontramos pequenos capacitores ao lado de cada
chip. São chamados de capacitores de desacoplamento (figura 1=
7).
Uma das caracteríticas elétricas =
dos
chips é que de um instante para outro podem aumentar substancialment=
e a
quantidade de corrente consumida. A fonte de alimentação nem
sempre tem condições de responder ao fornecimento de corrente=
com
a rapidez necessária (em geral em bilionésimos de segundo), e=
o
resultado é uma pequena queda de tensão próxima ao chip
que está solicitando este aumento de corrente. O capacitor de
desacoplamento tem condições de fornecer rapidamente a corren=
te
elevada que o chip exige, dando tempo à fonte para se adaptar ao novo
patamar de corrente. Os capacitores de desacoplamento funcionam portanto como pequenas baterias =
axiliares,
ajudando a fonte de alimentação no fornecimento de corrente p=
ara
os chips.
Um
capacitor não precisa necessariamente ter placas paralelas e um
dielétrico. Qualquer objeto possui uma capacitância. O corpo
humano, por exemplo, pode funcionar como um capacitor de baixo valor, mas a=
inda
assim capaz de armazenar cargas elétricas. É o que chamamos d=
e eletricidade
estática.
C=
apacitores
também têm grandes aplicações em circuitos de
rádio. Eles não permitem a passagem da corrente contín=
ua,
já que seu dielétrico é um isolante, mas permitem a
passagem de tensões alternadas. Como a corrente alternada trafega or=
a no
sentido direto, ora no sentido inverso, um capacitor pode ora se carregar
positivamente, ora negativamente, deixando que a corrente alternada o
“atravesse”. Quanto mais alta é a freqüência =
da
corrente alternada, mais facilmente ela atravessa o capacitor. Eles podem a=
ssim
ser usados como filtros, barrando as freqüências baixas e deixan=
do
passar as freqüências altas.
Q=
uando
são necessárias capacitâncias elevadas, são
utilizados capacitores eletrolíticos de alumínio ou
tântalo. Os capacitores eletrolíticos de alumínio
são muito usados em fontes de alimentação, em circuito=
s de
som, rádio e TV, e até em placas de computador. Entretanto pa=
ra
as placas de computador é mais recomendável usar os capacitor=
es
de tântalo. Eles são mais caros, porém são mais
duráveis e de menor tamanho. São muito usados em discos
rígidos e telefones celulares, mas também os encontramos sendo
usados como capacitores de desacoplamento do processador, nas placas de CPU.
Infelizmente para economizar, muitos fabricantes de placas de CPU usam
capacitores eletrolíticos de alumínio, ao invés de t&a=
circ;ntalo.
Isso poderia ser aceitável, se levassem em conta a vida útil =
do
capacitor. Existem capacitores eletrolíticos com duraçã=
;o
de 10.000 horas, outros com 5.000 horas, outros com apenas 1.000 horas, que
são mais baratos. Placas de CPU de baixo custo e baixa qualidade usam
muitos componentes inadequados, sobretudo capacitores de baixa qualidade.
Placas de CPU feitas por fabricantes comprometidos com a qualidade utilizam
capacitores de tântalo ou então eletrolíticos de
alumínio de longa duração.
Bobina<=
/span>
A=
bobina
é um componente elétrico construído por um fio enrolad=
o em
várias voltas. Seu valor é a indutância, e a uni=
dade
de medida é o henry<=
/span>
(H). Esta unidade é muito elevada para medir as bobinas da vida real,
portanto são mais utilizados o milihenry=
(mH) e o microhenry
(mH).
|
|
Figura
3.18
Bobinas
e seus símbolos
|
A=
bobina
é atravessada facilmente pela corrente contínua. Corrente
alternada de baixa freqüênica
também tem facilidade para atravessar uma bobina, mas quanto maior
é a freqüência, maior é a dificuldade. Esta
característica é inversa à do capacitor. Por isso,
associações de capacitores e bobinas são usados para formar filtros de vários tipos, com=
o por
exemplo, os sintonizadores. Quando giramos o botão sintonizador de
estações de um rádio (DIAL), estamos na verdade atuando
sobre um capacitor variável, associado a uma bobina, selecionado a
freqüência desejada.
Transfo=
rmador
Q=
uando
duas bobinas são enroladas sobre o mesmo núcleo, temos um
componente derivado, chamado transformador. Cada uma das bobinas
é chamada de enrolamento. Quando aplicamos uma tensão =
no
primeiro enrolamento (chamado de primário), podemos retirar u=
ma
outra tensão, sendo gerada pelo segundo enrolamento (secund&aacut=
e;rio).
Isto pode ser usado para aumentar ou reduzir a tensão. Em uma fonte =
de
alimentação convencional (não chaveada), o primeiro
circuito é um transformador, que recebe a tensão da rede
elétrica (110 ou 220 volts) e gera no secundário uma outra
tensão alternada, porém de menor valor.
|
|
Figura
3.19
Transformador
e seu símbolo
|
Os
transformadores têm muitas outras aplicações. São
usados por exemplo como isoladores da linha
telefônica =
em modems. Eles protegem (até c=
erto
ponto) o modem de eventuais sobretensões=
na
linha telefônica. Pelo fato de terem uma indutância, eles
também atuam como filtros de ruídos.
|
|
Figura
3.20
Transformador
usado em um modem.
|
Diodo
O=
diodo
é um componente classificado como semicondutor. Ele é
feito dos mesmos materiais que formam os transistores e chips. Este material
é baseado no silício. Ao silício são adicionadas
substâncias chamadas genericamente de dopagem ou impurezas<=
/i>.
Temos assim trechos tipo N e tipo P. A diferença entre os dois tipos
está na forma como os elétrons são conduzidos. Sem ent=
rar
em detalhes sobre microeletrônica, o importante aqui é saber q=
ue
quando temos uma junção PN, a corrente elétrica trafega
com facilidade do treho P para o trecho N, mas
não consegue trafegar no sentido inverso. O diodo possui seus dois
terminais ligados às partes de uma junção PN. A parte
ligada ao P é chamada de anodo, e a parte ligada ao N é
chamada de catodo. A corrente elétrica trafega livremente no
sentido do anodo para o catodo, mas não pode trafegar no sentido
inverso.
|
|
Figura
3.21
Diodos
e seu símbolo.
|
P=
or causa
desta característica, os diodos são usados, entre outras
aplicações, como retificadores. Eles atuam no processo=
de
transformação de corrente alternada em corrente contín=
ua.
LED
O=
LED
é um tipo especial de diodo que tem a capacidade de emitir luz quando
é atravessado por uma corrente elétrica. Como todo diodo, o L=
ED (Light Emitting Diode) permite a passagem de corrente (quando acende)=
no
sentido direto, do anodo para o catodo. No sentido inverso, a corrente
não o atravessa, e a luz não é emitida. =
|
|
Figura
3.22
LEDs<=
span
style=3D'font-size:10.0pt;font-family:Verdana'> e seu símbolo.
|
E=
xistem LEDs que emitem luz vermel=
ha,
verde, amarela e azul. Existem LED=
s
que emitem luz infravermelha, usados em sistemas de alarmes. Existem ainda =
os
que emitem luz vermelha ou verde, dependendo do sentido da corrente. S&atil=
de;o
na verdade dois LEDs=
, um
vermelho e um verde, ambos montados sobre a mesma base, e ligados em parale=
lo,
um no sentido direto e outro no inverso. Este tipo de LED é usado, p=
or
exemplo, em gravadores de CD-ROM. Quando estão lendo, emitem luz ver=
de
ou amarela. Quando estão gravando, emitem luz vermelha.
Display
numérico
A=
luz
emitida por um LED parte de um pequeno ponto luminoso, onde está a junção PN. Graças ao um difusor
ótico, que é uma semi-esfera, temos a sensação =
de
que a luz sai de todo o LED, e não apenas da junção PN.
Podemos ter difusores de vários formatos, inclusive retangulares. O
display digital com LEDs
é um conjunto com 7 LEDs, cada um deles =
com um
difusor retangular. Muitas vezes existe um oitavo LED que indica o ponto
decimal. Cada um dos segmentos do display pode ser aceso ou apagado
individualmente, e dependendo da combinação, diferentes
números são formados.
|
|
Figura
3.23
Display
digital formado por LEDs<=
/span>.
Este possui 4 dígitos.
|
U=
ma das
características do display digital formado por =
LEDs é sua alta luminosidade. Em
aplicações em que são usadas pilhas ou baterias, este =
tipo
de display tem um problema: o consumo de corrente é relativamente el=
evado
para a bateria. Mais eficiente é o display de cristal líquido,
que não é luminoso, mas seu consumo de corrente é muito
menor. As calculadoras e relógios digitais dos anos 70 usavam displa=
ys
com LEDs. As pilhas =
das
calculadoras ficavam logo gastas. Os relógios ficavam apagados, e era
preciso pressionar um botão lateral para acender o display e ver as
horas. Já nos anos 80, os displays de cristal líquido passara=
m a
ser mais comuns em calculadoras, relógios e em outros aparelhos
alimentados por baterias.
Transis=
tor
E=
ste
é sem dúvida o mais importante componente eletrônico
já criado. Ele deu origem aos chips que temos hoje nos computadores.=
Um
processador, por exemplo, tem no seu interior,
vários milhões de microscópicos transistores. Inventado
nos laboratórios Bell nos anos 40, o transistor é um substitu=
to
das velhas válvulas eletrônicas, com grandes vantagens: tamanho minúsculo e pequeno consumo de energia.=
A
figura 24 mostra alguns transistores e seu símbolo eletrônico.
Note que existem vários tipos de transistores. Quanto ao sentido da
corrente elétrica, os transistores são classificados como NPN=
e
PNP, ambos mostrados na figura 24.
|
|
Figura
3.24
Transistores
e seus símbolos
|
Os
transistores realizam inúmeras funções, sendo que as m=
ais
importantes são como amplificadores de tensão e amplificadore=
s de
corrente. Por exemplo, o sinal elétrico gerado por um microfone &eac=
ute;
tão fraco que não tem condições de gerar som qu=
ando
é aplicado a um alto falante. Usamos então um transistor para
elevar a tensão do sinal sonoro, de alguns milésimos de volts
até alguns volts. Seria tensão suficiente para alimentar um a=
lto
falante, mas ainda sem condições de fornecer a potência
adequada (a tensão está correta mas a
corrente é baixa). Usamos então um segundo transistor atuando
como amplificador de corrente. Teremos então a tensão igual
à gerada pelo primeiro transistor, mas com maior capacidade de forne=
cer
corrente.
Os
aumentos de tensão e de corrente são no fundo, aumentos de
energia. Esta energia não é gerada a partir do nada. O transi=
stor
retira a energia necessária a partir de uma bateria ou fonte de
alimentação. A figura 25 mostra o diagrama do circuito simple=
s, com
dois transistores, para amplificar o sinal gerado por um microfone para que
seja aplicado em um alto falante. Note que os transistores não traba=
lham
sozinhos. Eles precisam ser acompanhados de resistores, capacitores, e
dependendo do circuito, outros componentes, para realizar suas
funções.
|
|
Figura
3.25
Amplificador
transistorizado.
MIC =3D Microfone
AF1 =3D Alto falante
VCC =3D Terminal positivo da bateria que alimenta o circuito
GND =3D Terra, ou terminal negativo da bateria.
|
E=
xistem transitores de baixa, média e alta potên=
cia.
Quanto maior é a potência, maior é o seu tamanho. Os
transistores de alta potência em geral precisam ser montados sobre
dissipadores de calor (coolers). Existem transitores especializados em operar com
freqüências de áudio e outros especializados em altas
freqüências, usados em circuitos de rádio e TV. Existem
transistores especializados em chaveamento, indicados para operar em circui=
tos
digitais. Existem fototransistores, que amplifi=
cam o
sinal gerado pelo seu sensor ótico. Enfim, existem milhares de tipos=
de
transistores, para as mais variadas aplicações.
Regulad=
or de
voltagem
T=
odos os
circuitos eletrônicos necessitam, para que funcionem corretamente, do
fornecimento de corrente vinda de uma bateria ou fonte de
alimentação com valor constante. Por exemplo, se um circuito =
foi
projetado para funcionar com 5 volts, talvez pos=
sa
funcionar com tensões um pouco maiores ou um pouco menores, como 5,5=
V
ou 4,5 V, mas provavelmente não funcionará corretamente com
valores muito mais altos ou muito mais baixos, como 6 V ou 4 V. Uma fonte de
alimentação precisa portanto gerar uma tensão constant=
e, independente
de flutuações na rede elétrica e independente da
quantidade de corrente que os circuitos exigem. Por isso todas as fontes de=
boa
qualidade utilizam circuitos reguladores de voltagem.
&=
Eacute;
possível criar um regulador de voltagem utilizando alguns transistor=
es, resitores e um componente especial chamado diodo <=
span
class=3DSpellE>Zener, capaz de gerar uma tensão fixa de
referência a ser “imitada” pela fonte. Os fabricantes
construíram esses circuitos de forma integrada, semelhante a um chip,
usando uma única base de silício. Os reguladores mais simples
têm um encapsulamento parecido com o de um
transistor de potência, com três terminais. Um dos terminais
é o terra, que deve ser ligado ao terminal
negativo da fonte. O outro terminal é a entrada, onde deve ser aplic=
ada
a tensão bruta, não regulada. O terceiro terminal é a
saída, por onde é fornecida a tensão regulada. A
tensão de entrada deve ser superior à tensão que vai s=
er
gerada. O regulador “corta” uma parte desta tensão de mo=
do a
manter na saída uma tensão fixa. Por exemplo, para alimentar =
um
regulador de +5 Volts, podemos aplicar na entrad=
a uma
tensão não regulada de +8 Volts, podendo variar entre +6 e +<=
st1:metricconverter
ProductID=3D"10. A" w:st=3D"on">10. A saída
fornecerá +5 V, e o restante será desprezado. <=
/p>
|
|
Figura
3.26
Reguladores
de voltagem em uma placa de CPU.
|
M=
uitos
reguladores produzem tensões fixas, mas existem modelos que podem ser
ligados a uma tensão de referência que pode ser programada. Nas
placas de CPU existe um circuito responsável por gerar as tens&otild=
e;es
exigidas pelo processador. A maioria dos processadores modernos requer uma
fonte de +3,3 V para operações externas, e uma fonte de valor
menor para as operações internas. Dependendo do processador, =
esta
tensão pode ser de +1,3 V, +1,6V, +1,7V, +2,1V ou praticamente qualq=
uer
valor entre 1 V e 3,5 V. Nos processadores mais =
novos,
esses valores tendem a ser menores, em geral inferiores a 2 V. O circuito
gerador de voltagem da placa de CPU toma como base a tensão de +3,3 V
fornecida pela fonte de alimentação do computador, e em
função do valor indicado pelo processador, gera a tensã=
;o
necessária. Trata-se de um regulador de tensão variáve=
l e
programável.
Soquete=
s
A=
maioria
dos componentes eletrônicos são soldados nas suas placas. Outr=
os
componentes precisam ser removidos periodicamente para
substituição ou manutenção. Por exemplo, uma
lâmpada não é aparafusada ou soldada diretamente aos fi=
os
da rede elétrica. Ela é presa através de um bocal, e e=
ste
sim é aparafusado aos fios. O bocal é na verdade um soquete p=
ara
a lâmpada, tanto que em inglês, é usado o termo socket para designar o bocal de uma lâmp=
ada.
D=
a mesma
forma, certos componentes eletrônicos podem precisar ser removidos,
trocados ou instalados. É o caso dos processadores, memórias e
alguns chips. Para isso esses chips são encaixados sobre soquetes=
.
Os soquetes sim, são soldados nas placas de circuito, e sobre eles
encaixamos os chips.
O=
tipo
mais simples é o chamado de soquete DIP (dual in-line
package). Ele é apropriado para chips que
também usam o encapsulamento DIP. Existem
soquetes DIP de vários tamanhos, com diferentes números de te=
rminais
(ou pinos). Podemos encontrar soquetes DIP com 8, 10, 12, 14, 16, 18, 20, 2=
2,
24, 28 pinos, e assim por diante. Em geral soquetes com mais de 32 pinos
são mais largos que os com menos pinos. Na própria figura 28
vemos duas versões de soquetes de 28 pinos, sendo um largo e um
estreito.
|
|
Figura
3.28
Soquetes
de vários tamanhos.
|
T=
odos os
pinos dos soquetes são numerados, porém esta
numeração não está indicada, mas fica
implícita. Para saber o número de qualquer pino, basta locali=
zar
a posição do pino 1. Tanto os soquetes quanto os chips de encapsulamento DIP possuem uma extremidade diferente =
da
outra, com um chanfro ou algum tipo de marcação. Muitas vezes
esta marcação está desenhada na placa (os desenhos na
placa são chamados de serigrafia). Quando olhamos um soquete =
de
tal forma que o chanfro ou marcação fique orientada para a
esquerda, o pino 1 é o primeiro na parte inferior (veja a figura 29)=
. Os
demais pinos seguem a seqüência, até a outra extermidade. No outro lado da mesma extremidade a
seqüência continua, até o último pino do soquete, =
que
fica na mesma extremidade que o pino 1.
|
|
Figura
3.29
Numeração
de alguns soquetes DIP.
|
Q=
uando
vamos encaixar um chip em um soquete, temos que prestar atençã=
;o
na orientação correta. O pino 1 do chip deve corresponder ao =
pino
1 do soquete. Se o encaixe for feito de forma invertida ou deslocada, o chip
provavelmente queimará, e o mesmo pode ocorrer com a placa. Os chips
também possuem um chanfro ou um ponto circular em baixo relevo para
indicar a posição do pino 1, e a seqüência é=
; a
mesma do soquete (figura 30).
|
|
Figura
3.30
Posição
do pino 1 nos chips.
|
Os
soquetes mais sofisticados são os dos processadores. Possuem mais de=
300
pinos, alguns ultrapassando os 400. O número de pinos é
tão grande que o encaixe se torna difícil. Cada pino requer u=
ma
pequena força para entrar sob pressão no furo correspondente =
do
soquete, mas quando multiplicamos esta pequena força por 400, temos =
uma
grande força. Como seria difícil encaixar e retirar o chip do
soquete, foram adotados para esses casos os soqu=
etes
de força de inserção zero (Zero Insertion
Force, ou ZIF). Eles possuem uma pequena alavanca lateral que ao ser aberta
aumenta os furos onde os terminais (“perninhas”) do chip v&atil=
de;o
ser encaixados. O chip é posicionado com facilidade e então a
alavanca é travada fazendo com que cada furo diminua e segure o term=
inal
correspondente com boa pressão.
|
|
Figura
3.31
Encaixando
um processador em um soquete ZIF.
|
E=
m todos
os processadores modernos, existem mecanismos que impedem que o encaixe seja
feito de forma invertida. Existem por exemplo, furos a menos em um ou dois
cantos do soquete, bem como pinos a menos em um ou dois cantos do processad=
or,
fazendo com que o encaixe só possa ocorrer na posição
certa.
|
|
Figura
3.32
Furações
diferentes no processador e no soquete ZIF impedem o encaixe invertido.
|
D=
evemos entretanto tomar cuidado com certos processadores ant=
igos.
Os processadores 486 e 586 não possuem diferenças entre as
posições de encaixe, portanto um usuário distraí=
;do
conseguirá fazer o encaixe de 4 formas diferentes, sendo uma correta=
e 3
erradas. As formas erradas causarão a queima do processador. Devemos=
portanto prestar atenção no chanfro exi=
stente
no processador. Um dos seus cantos é diferente dos outros, e este de=
ve
corresponder ao pino 1 do soquete. O pino 1 do soquete, por sua vez, &eacut=
e;
aquele mais próximo da “dobradiça” da alavanca. <=
/span>
|
|
Figura
3.33
Orientação
correta de processadores 486 e 586. As setas indicam a posiç&atild=
e;o
do pino 1.
|
D=
e um
modo geral, vários chips possuem pinos simétricos e por isso
podem ser indevidamente encaixados de forma errada, causando sua queima. Ao
fazer o encaixe temos sempre que procurar uma indicação de pi=
no 1
no soquete ou na serigrafia, e a indicação de pino 1 no chip.
Esta indicação é sempre apresentad=
a na
forma de um canto diferente ou marcado com um ponto. Preste
atenção também na posição do chanfro
existente no chip.
|
|
Figura
3.34
Indicações
de pino 1 em um chip e no seu soquete.
|
Slot
O=
slot é um tipo especial de soquete. A diferen&=
ccedil;a
é que normalmente são usados para o encaixe de placas, apesar=
de
serem usados também para certos processadores. A figura 35 mostra al=
guns
slots encontrados em placas de CPU.
|
|
Figura
3.35
Slots de uma placa de CPU.
|
U=
m slot é um conector plástico com uma, du=
as ou
três fendas alinhadas, nas quais existem internamente, duas
seqüências de contatos elétricos. A placa a ser conectada
possui contatos em ambas as faces, que correspondem a contatos nessas duas
fileiras do slot.
E=
ntre
1997 e 2000, os principais processadores foram produzidos em versões
para encaixe em slots. Eram os
processadores Pentium II, bem como as primeiras versões dos processa=
dores
Celeron, Pentium III e Ath=
lon.
As placas de CPU correspondentes tinham slots
próprios par ao encaixe desses processadores. Este método de
encaixe caiu em desuso, mas dependendo das características de futuros
processadores, nada impede que venham a ser novamente adotados. O
próprio processador Intel Itanium e seus
sucessores serão produzidos inicialmente em versões de cartuc=
ho.
|
|
Figura
3.36
Slot para processador.
|
N=
ormalmente
os slots possuem dispositivos que impedem que s=
eja
feito o encaixe de forma invertida, ou que seja encaixada uma placa n&atild=
e;o
compatível com o slot. Por exemplo, n&at=
ilde;o
conseguiremos instalar uma placa de vídeo AGP em um slot
PCI pois a chapa traseira do gabinete do computa=
dor
impedirá o posicionamento da placa. Processadores Pentium II, Pentium
III e Celeron não podem ser encaixados e=
m um slot para processador Athlon, e
vice-versa, mas um usuário distraído pode conseguir posiciona=
r o
processador de trás para frente, queimando tanto o processador como a
placa. Instalar processadores não é tarefa para leigos. &Eacu=
te;
preciso saber reconhecer os processadores e também saber os modelos =
suportados
por cada placa de CPU.
Conecto=
res
Um
conector é uma peça contendo um grupo de contatos
elétricos relacionados uns com os outros. Por exemplo, na extremidad=
e do
cabo que parte do monitor, existe um conector de 15 pinos que é liga=
do
em outro conector correspondente da placa de vídeo. Os sinais existe=
ntes
nesses 15 pinos são diferentes, mas estão relacionados entre =
si.
Existem por exemplo 2 pinos para a transmissão do vermelho, 2 para o
verde e 2 para o azul. Existem pinos para transmissão do sincronismo
horizontal e sincronismo vertical.
|
|
Figura
3.37
Conectores
do monitor e da placa de vídeo.
|
M=
uitos
conectores são internos, outros são externos. Os internos
são usados para conexões dentro do computador. Os externos
são usados para ligar dispositivos externos. Conectores trabalham aos
pares, e normalmente um é chamado “macho” e o outro “fêmea”. Obviamente o tipo m=
acho
é aquele com pinos metálicos, que se encaixam sobre os
orifícios metalizados do conector fêmea
correspondente. Realmente tem uma certa
conotação sexual.
E=
ntre os
conectores externos, citamos os da impressora, do teclado, do mouse, do joystick, da rede elétrica, do modem, das caix=
as de
som e microfones e diversos outros. Todos serão apresentados em part=
es
oportunas deste livro. Os conectores internos também são
diversos: da fonte de alimentação, do disco rígido, do=
drive de disquetes, do drive de
CD-ROM, e assim por diante. Um conector muito importante é o do cabo=
que
liga o disco rígido à sua interface (figura 38). Trata-se de =
um
conector macho de 40 pinos, encontrado na placa de CPU. Observe que em qual=
quer
caso existe a indicação da posição do pino 1 de=
ste
conector.
|
|
Figura
3.38
Conector
da interface IDE e a posição do pino 1<=
/span>.
|
No
conector da interface do disco rígido, encaixamos um cabo que leva os
sinais até o disco rígido propriamente dito. Em uma das extre=
midades
deste cabo existe um conector fêmea correspondent=
e.
Este conector é ligado a aquele existente na placa de CPU, e temos q=
ue
prestar atenção na posição do pino 1. Basta
observar que um dos fios do cabo é pintado de vermelho. A
posição do fio vermelho corresponde ao pino 1 do conector do
cabo, que deve estar alinhado com o pino 1 do conector existente na placa.
|
|
Figura
3.39
Um
dos fios do cabo é pintado, geralmente de vermelho, o que indica a
posição do pino 1.
|
Cabo fl=
at
A=
lguns
dispositivos são ligados diretamente aos outros, usando apenas
conectores. O processador, as memórias e os chips são encaixa=
dos
diretamente em seus soquetes. As placas de expansão são
conectadas diretamente nos seus slots. Existem<=
span
class=3DGramE> entretanto vários casos de conexões
elétricas que precisam ser feitas através de cabos. Por exemp=
lo,
o disco rígido não pode ser ligado diretamente na placa de CP=
U.
Um cabo apropriado é então usado para esta conexão. O
mesmo ocorre com o drive de CD-ROM, drive de disquetes e vários outros dispositivo=
s.
Quando o número de sinais elétricos do conector é muito
grande, a forma mais eficiente de realizar a conexão é utiliz=
ando
o chamado cabo flat. Existem cabos flat com diversos números =
de
condutores. O cabo usado para o drive de disque=
tes
usa 34 vias. Os cabos usados em discos rígidos I=
DE
usam 40 ou 80 vias. Os cabos usados por discos e dispositivos SCSI p=
odem
usar 50, 68 ou 80 vias. Enfim, são vários padrões para
diversas aplicações. Os cabos flat possuem no mínimo d=
ois
conectores, que ligam um dispositivo à sua interface. Certas interfa=
ces
permitem ligar dois ou mais dispositivos, portanto os cabos flat
correspondentes possuem dois ou mais conectores.
|
|
Figura
3.40
Cabo flat para discos rígidos IDE.
|
T=
odos os
cabos flat possuem um dos seus fios pintado de vermelho (em alguns casos de
outra cor). Este é o fio número 1, que corresponde ao pino 1 de cada conector, que por sua vez têm que
corresponder aos pinos 1 dos conectores onde são encaixados.<=
/p>
Jumpers e microchaves
A=
microchave ou dip switch é um dispositivo que desempenha a mesma
função que o jumper. A diferen&cc=
edil;a
é que seu formato é similar ao de um chip. Além disso,=
as microchaves são apresentadas em grupos, em ger=
al de
4 ou 8 chaves. Cada chave pode ser posicionada nas posições O=
N e
OFF, o que equivale a configurações com jumper
e sem jumper, respectivamente.
O=
s jumpers e microchaves pos=
suem
várias aplicações. Nas placas de CPU, servem para
habilitar e desabilitar o funcionamento da bateria, selecionar o tipo e a
velocidade das memórias, a velocidade e a tensão do processad=
or,
entre varias outras funções.
Cristal=
T=
odos os
circuitos digitais dependem de uma base de tempo para poderem funcionar. Por
exemplo, um relógio digital precisa de um circuito capaz de gerar pu=
lsos
digitais a cada centésimo de segundo. Nesse caso, 100 desses pulsos
correspondem a 1 segundo, e a partir daí são feitas contagens=
de
minutos, horas, etc. Outros circuitos digitais também necessitam de
geradores de base de tempo similares. O cristal é o componente respo=
nsável
pela geração da base de tempo. Cristais são produzidos
para entrar em ressonância em uma determinada freqüência. =
Eles
são muito precisos nesta tarefa. São capazes de gerar
freqüências fixas, com precisão da ordem de 0,001%.
Os
cristais são muito sensíveis, por isso são protegidos =
por
um encapsulamento metálico. A figura 44 =
mostra
alguns cristais encontrados nas placas de um computador.
Gerador de clock
Um
cristal não trabalha sozinho na geração de
freqüências que mantém a cadência de funcionamento =
dos
circuitos digitais. São usados circuitos chamados osciladores=
, e
o cristal serve apenas como a referência para esses circuitos. Existem
chips que são capazes de gerar diversos valores de
freqüência, a partir de um cristal de referência. Um circu=
ito
oscilador gera uma única freqüência. Já um circuito
gerador de clock é capaz de gerar
vários valores de freqüências, e cada uma delas pode ser
programada, ou seja, seu valor pode ser escolhido entre várias
opções. Por exemplo, certas placas de CPU podem utilizar
processadores com clocks externos de 66, 100 ou=
133
MHz. O valor escolhido é determinado através da
programação do gerador de clock. =
|
|
Figura
3.45
Um
chip gerador de clock.
|
Compone=
ntes
SMD
A=
ntigamente
a montagem de uma placa de circuito era um processo extremamente demorado e
precisava ser feito manualmente. Os componentes eram encaixados em furos
existentes nas placas, e a seguir eram soldados. Eram necessárias
várias horas para realizar este trabalho, e o custo final era muito
elevado, já que o trabalho consumia muita mão de obra. Hoje em
dia é utilizado um processo muito mais rápido, graças
à tecnologia SMD (Surface Mounted
Devices, ou dispositivos montados na
superfície). Os componentes não têm mais terminais para
serem encaixados em furos das placas de circuito. Ao invés disso, el=
es
são colocados sobre a superfície da placa. Uma camada de past=
a de
solda (resina com minúsculas partículas de solda em estado
sólido) é previamente aplicada sobre a placa, ainda sem
componentes. A seguir uma grande máquina coloca os componentes SMD n=
os
seus lugares. A placa é encaminhada para um forno que derrete a past=
a de
solda, fixando definitivamente os componentes.
O=
gerador
de clock mostrado na figura 45, bem como os peq=
uenos
componentes ao seu redor, são do tipo SMD=
. Eles
não têm “perninhas” (ou terminais) como os compone=
ntes
convencionais. São indicados para produção de pe&ccedi=
l;as
em alta escala, enquanto os componentes convencionais são indicados =
para
montagem em pequena escala.
Voltage=
ns e
bits
U=
ma das
características mais importantes dos circuitos digitais é a
representação dos bits 0 e 1 através de dois valores de
tensão. Em geral é usado um valor pequeno, entre 0 e 0,3 volts, para indicar o bit 0, e um valor um pou=
co
maior, da ordem de alguns poucos volts, para indicar o bit 1. Por exemplo,
típicos chips de memória usam cerca de 0,2 V para representar=
o
bit 0 e em torno de 2,4 V para representar o bit “1”. Valores
diferentes podem ser usados, dependendo da tecnologia. Por exemplo, no inte=
rior
dos processadores modernos, os niveis de
tensão são ainda mais baixos. São usados internamente
valores em torno de 1,=
0 a
1,5 volts para representar o bit 1, e um valor sempre próximo de 0 V
para representar o bit 0. Seja qual for o caso, o nível de tens&atil=
de;o
que representa o bit 0 será sempre um valor positivo, apesar de muito
pequeno. Da mesma forma, o nível de tensão que representa o b=
it 1
será sempre um valor um pouco menor que a tensão da fonte de
alimentação. A maioria dos chips existentes nas placas modern=
as
opera com alimentação de 3,3 volts, mas muitos já oper=
am
com apenas 2,5 volts. Há alguns anos atrás a maioria dos chips
operavam com 5 volts.
T=
eoricamente
quaisquer níveis de voltagem poderiam ser usados para representar os
bits 0 e 1. Na prática são usados valores pequenos, para que o
consumo de energia e a dissipação do calor também sejam
pequenos, principalmente nos computadores. Valores maiores podem ser
encontrados em alguns cicuitos. Por exemplo, em=
um
relógio despertador digital alimentado por uma bateria de 9 volts, o=
bit
1 pode ser representado por um valor superior a 8 volts, e o bit 0 por um v=
alor
menor entre 0 e 1 volt.
|
|
Figura
3.46
Medindo
as tensões que representam os bits em um chip alimentado por 3,3
volts.
|
A=
figura
46 mostra uma medida teórica das tensões em pinos de um chip,
representando bits 0 e 1. O pino que apresenta a tensão de 0,13 volts
corresponde a um bit 0. Os outros dois pinos indicados, com tensões =
de
2,83V e 2,74V representam bits 1. Os valores de tensão que represent=
am
os bits podem variar sensivelmente de um chip para outro, ou mesmo de um pi=
no
para outro. Não existe um valor exato, e sim, uma faixa de valores.<=
/span>
Na
prática esta medida nem sempre pode ser feita com um multímet=
ro.
Quando um chip está trabalhando, seus bits estão variando
rapidamente, entre 0 e 1. Um multímetro não é capaz de
medir tensões variáveis em alta velocidade, é adequado=
a
medir apenas tensões constantes. Supondo que este chip esteja fornec=
endo
bits constantes, mediríamos valores como os da figura 46. Em alguns
casos um chip pode realmente apresentar valores constantes. Por exemplo, o =
chip
que contém a interface de impressora pode transmitir bits
variáveis enquanto está sendo produzida uma listagem, mas ao
terminar, pode manter fixo em suas saídas o código biná=
;rio
do último dado enviado para a impressora. Neste ponto poderámos fazer uma medida usando o
multímetro, como a apresentada na figura 46.
O=
bserve
na figura 46 mais um detalhe importante sobre os níveis de tens&atil=
de;o
que representam os bits. Os valores especificados não são exa=
tos,
e sim, valores extremos. Por exemplo, um fabricante de memórias pode
especificar:
VOHmin =3D 2,4 V
VOLmax =3D 0,4 V
S=
ignifica
que a tensão de saída nos seus terminais que representa o bit=
1 (Voltage Output High) &eac=
ute; de
no mínimo 2,4 volts. Pode assumir valores maiores, como no exemplo da
figura 46, onde medimos 2,83 e 2,74 volts. Da mesma forma, este fabricante
especifica que a tensão de saída que representa o bit 0 (Voltage Output Low) &eacu=
te; de
no máximo 0,4 volts. Pode assumir valores
menores, como os 0,13 volts indicados na figura. Os projetistas de hardware
sempre levam em conta faixas de valores, tensões máximas e
mínimas, e assim por diante.
Tristate ou alta impedância
Q=
uando um
circuito digital está em operação normal, pode gerar na
sua saída, tensões correspondentes aos bits 0
e 1. Existe entretanto um terceiro estado no qual um circuito pode operar.
É o chamado terceiro estado (tristate)
ou alta impedância. Em inglês são usados
também os termos high impedance ou float
(flutuar). É como se o circuito estivesse desconectado. Imagine por
exemplo dois módulos de memória, cada um
encaixado em seu respectivo soquete. Digamos que cada um desses
módulos tenha 64 MB. Quando o processador acessa um endereço =
de
memória entre 0 e 64 MB, o primeiro módulo está ativo =
e o
segundo fica =
em tristate. Quando é acessado =
um
endereço superior a 64 MB, e até 128 MB, o segundo mód=
ulo
estará ativo e o primeiro estará em tristate. O
uso do terceiro estado é necessário para que dois ou mais
circuitos possam operar ligados ao mesmo ponto, ou ao mesmo barramento,
porém apenas um de cada vez deverá entregar seus bits, e os
demais devem ficar como se estivessem desligados. No terceiro estado, os
circuitos estão energizados, mas sua
resistência elétrica torna-se tão elevada que consomem =
uma
corrente desprezivelmente pequena, não afetando o funcionamento dos
demais circuitos. É como aquele velho ditado, “quando um burro=
fala
o outro abaixa a orelha”. O burro que está falando é o
circuito ativo, gerando seus bits. Os burros de orelhas abaixadas sã=
o os
circuitos que estão no terceiro estado.
E=
xistem
vários exemplos de uso do terceiro estado. Um deles é o uso do
DMA (acesso direto à memória). Em condições
normais, o processador gera os endereços e os sinais de controle da
memória. Quando é feita uma transferência de dados por =
DMA,
o processador entra em tristate e deixa que o
circuito controlador de DMA (que na verdade faz parte do chipset)
realize a transferência, gerando seus próprios endereço=
s e
sinais de controle para a memória. Quando o processador está =
em
uso normal, o controlador de DMA fica em tristate.
O=
utro
exemplo: várias placas de expansão estão conectadas no=
barramento PCI de uma placa de CPU, e todas elas podem
transmitir dados através do seu slot, porém elas não podem fazer
transmissões no mesmo instante. No instante em que uma placa envia d=
ados
(ou que o processador comanda uma leitura dos seus dados), as
demais placas mantém suas saídas em tristate.
A=
maioria
dos chips tem a capacidade de entrar em tristat=
e.
Eles possuem um pino (ou seja, uma “perninha”)
chamado CS, ou chip select. Quando este sinal
está ativado, o chip está em uso normal. Quando este sinal
é desativado, o chip entra em tristate.<=
/span>
Diagram=
as de
tempo
C=
omo mencionamos, os bits representados pelos circuitos dig=
itais
variam bastante ao longo do tempo. Por exemplo, em um moderno chip de
memória, os bits podem variar mais de 100 milhões de vezes a =
cada
segundo, ora representando 0, ora representando 1. Um diagrama de tempo
é um gráfico simplificado que mostra os valores dos bits ao l=
ongo
do tempo, como o vemos na figura 47.
|
|
Figura
3.47
Diagrama
de tempo.
|
Um
diagrama de tempo pode representar um ou vários sinais digitais
simultaneamente. Neste caso é usado um único eixo Y,
representando o tempo, e vários eixos X independentes, cada um deles
representando um sinal digital diferente. Cada sinal digital por sua vez as=
sume
valores 0 e 1 ao longo do tempo. O diagrama da figura 47 representa dois si=
nais
digitais. Neste diagrama podemos observar, além dos trechos nos quai=
s o
circuito gera bits 0 e 1, um pequeno intervalo de
tempo em cada transição de 1 para 0 ou de 0 para 1, represent=
ados
por trechos inclinados do gráfico. Esta transição deve=
ria
ser instantânea, do ponto de vista matemático, mas na pr&aacut=
e;tica
leva um certo tempo, bastante pequeno, Por exemp=
lo, um
chip que gera bits diferentes a cada 10 ns (10 bilionésimos de segun=
do)
pode demorar entre 1 e 2 ns para mudar seu estado de 0 para 1 ou de 1 para =
0.
O=
bserve
ainda que um diagrama de tempo não é a
mesma coisa que um gráfico de tensão ao longo do tempo. Um
gráfico de tensão ao longo do tempo mostra os valores de
tensão existentes em um ponto de um circuito, e não os bits q=
ue
representam. A figura 48 mostra um exemplo de gráfico de tensã=
;o
ao longo do tempo, com todas as suas imperfeições. Este tipo =
de gráfico
pode ser visualizado através de um aparelho chamado oscilosc&oacu=
te;pio,
usado em laboratórios de eletrônica.
|
|
Figura
3.48
Gráfico
de voltagem ao longo do tempo.
|
No
gráfico da figura 48, a
tensão começa com um valor baixo, representando um bit 0. No
instante T1 começa a transição para representar um bit=
1.
O gráfico assume um trecho crescente e rápido, mas não=
se
estabiliza imediatamente no seu valor máximo. A tensão atinge
momentaneamente um valor máximo, em T2. A seguir reduz oscilando
até se estabilizar em um valor definitivo, ou
então limitada em uma faixa pequena. Este fenômeno &eac=
ute;
chamado de overshoot. No instante T3 o <=
span
class=3DSpellE>overshoot terminou ou foi reduzido a um valor que
não afeta os circuitos e a tensão é considerada
estabilizada. No instante T4 começa a transição de 1 p=
ara
0, que termina em T5. Segue-se um trecho em que a tensão já t=
em o
valor 0, mas ainda não estabilizou no seu valor definitivo. Este tre=
cho
é o undershoot, e dura até=
o
instante T6.
E=
xistem
outras imperfeições mesmo nos trechos em que a tensão
está estabilizada há “bastan=
te
tempo” em va=
lores Low e High (0 e
1). Essas imperfeições são chamadas de ripple
(em português, ruído). São u=
ma
espécie de interferência vinda da fonte de
alimentação e de circuitos adjacentes. Quando dois circuitos
estão próximos, transições binárias em um
deles pode irradiar ondas eletromagnética=
s que
produzem interferências captados pelo outro. Essa=
s interferências
também pode chegar da própria fonte de
alimentação. Quando um chip faz transições
rápidas entre bits 0 e 1, seu consumo de
corrente pode variar na mesma velocidade, e a fonte de
alimentação, ao tentar suprir esta variação de
corrente, pode sofrer uma pequena variação nas suas
saídas. É o ripple da fonte de
alimentação, que é propagado para todos os demais
circuitos. O ripple não pode ser muito
acentuado, caso contrário irá comprometer os valores dos bits=
.
E=
m um
circuito digital bem projetado, o overshoot e o=
undershoot devem assumir proporções
não muito exageradas para que não impeçam o correto
funcionamento dos chips. Isto é conseguido com o uso de uma fonte de
alimentação bem projetada, com capacitores de desacoplamento =
ao
lado de cada chip e utilizando técnicas apropriadas para o
traçado das trilhas do circuito impresso da placa. Respeitadas essas
condições, o projetista não precisa se precisa se
preocupar com o overshoot, com o undershoot
nem com o ripple da fonte de
alimentação, mas precisa se preocupar com o tempo gasto nas
transições binárias, ou seja, nas mudanças de 0
para 1 e de 1 para 0. Por isso são usados os diagramas de tempo, onde
são indicados os trechos inclinados que representam as transiç=
;ões,
mas não são mostrados os detalhes como o=
vershoot,
undershoot e ripple=
.
D=
urante o
projeto de um circuito digital, o projetista deve inicialmente desenvolver =
uma
fase na qual é levada em conta a qualidade das tensões dos
circuitos. O ripple deve ser baixo, assim como =
o overshoot e o undershoot.=
Deve
ser levado em conta o valor, o tipo e a qualidade dos capacitores de
desacoplamento ligados em cada chip. Deve ser levada em conta a qualidade da
fonte de alimentação e o traçado das trilhas de circui=
to
da placa. O leitor pode não ser um projetista de placas, mas aqui po=
de
entender como a baixa qualidade da fonte e dos capacitores, aliado a um
traçado mal feito, contribuem para a ocorrência de erros que se
manifestam no mau funcionamento do computador.
|
|
Figura
3.49
Glitch. O surgimento de um “pico de voltagem”
indevido, mostrado no gráfico tensãoxt=
empo
acima, corresponde a um bit 1 indevido que sur=
ge
rapidamente, voltando a zero. Sendo indevidamente gerado, provoca resulta=
dos
indevidos no funcionamento do circuito digital.
|
A=
figura
49 mostra uma outra imperfeição nas tensões de um circ=
uito
digital. É o que chamamos de glitch.
Trata-se de uma interferência na qual o valor de tensão especi=
ficado
é momentaneamente alterado no sentido do bit oposto, produzindo uma
variação binária indesejável. O glitch
pode ocorrer quando o overshoot ou o undershoot são muito exagerados, ou quando um
capacitor de desacoplamento está mal dimensionado ou defeituoso, ou
mesmo quando existe um erro de projeto. Um circuito digital que recebe na s=
ua
entrada uma tensão com glitch vai
entendê-lo como uma transição binária que na ver=
dade
não existe. O resultado é o mau funcionamento do circuito.
Você certamente já viu a palavra glitch
no cinema mas talvez não se lembre. No fi=
lme Robocop 1 (versão legendada), aquele imenso
robô aponta a metralhadora para um funcionário da OCP e diz
“Polícia de Detroit, largue a arma, você tem 30
segundos...”. A seguir, mesmo depois que o sujeito joga a arma no
chão, o robô avisa: “Você tem 20 segundos.. você tem 10 segundos”, então met=
ralha
o infeliz (aliás, que filme ruim...). O responsável pelo
robô explica-se ao presidente da empresa: “foi apenas um glitch...”.
D=
epois de
garantir que o circuito tem tensões estáveis, com
imperfeições mínimas e sem glitch=
,
o projetista passa a uma fase em que leva em con=
ta
apenas os valores binários e os períodos de
transição. Essas são portanto as
informações apresentadas nos diagramas de tempo.
|
|
Figura
3.50
Convenções
usadas em um diagrama de tempo.
|
A=
figura
50 mostra alguns símbolos de eventos encontrados em diagramas de tem=
po:
a) Trigger positivo
Este
símbolo indica que no instante em que um sinal digital sofre uma
transição de 0 para 1, um evento ou mudança em outro s=
inal
digital será ativado.
b) Trigger negativo
Similar ao
positivo, exceto que o evento é disparado na transição
binária de 1 para 0.
c)
Retardo entre dois sinais
Mostra a
dependência temporal entre dois sinais relacionados. É usado
quando é informação relevante saber que um determinado
sinal será ativado depois de um determinado tempo a partir do qual o
primeiro é ativado.
d)
Indicação de barramento
Para evitar=
que
um diagrama fique muito extenso, podemos agrupar
vários sinais relacionados em um único eixo. Usamos para
representar, por exemplo, o barramento de dados=
do
processador ou memória, o barramento de
endereços, o conjunto de dados que estão trafegando
através de uma interface. Não existe interesse em especificar=
o
valor individual de cada um dos sinais digitais. Eles formam um grupo, e al=
guns
deles podem ser 1 e outros serem 0, e o circuito
funcionará independentemente dos valores.
e)
Mudança de estado em ponto indeterminado
Todos os
circuitos digitais apresentam pequenas variações, mas os
fabricantes sempre especificam valores máximos e mínimos. Por
exemplo, um determinado circuito pode apresentar um tempo médio de r=
esposta
de 15 ns, mas alguns componentes podem chegar a 10 ns, outros a 20 ns. Em
certos casos o projetista precisa compatibilizar seu circuito com component=
es
mais lentos e mais rápidos. Neste caso precisa levar em conta o prim=
eiro
instante e o último instante em que um sinal digital pode ser ativad=
o.
f) Don’t care
Significa
“não importa”. O sinal digital poderá ter neste
período, qualquer valor (obviamente, 0 ou 1), sem afetar o funcionam=
ento
do circuito. Por exemplo, se fizermos o diagrama da transmissão de d=
ados
por uma interface paralela, este diagrama deve começar indicando o d=
ado
que estava presente nas saídas da interface antes de começar a
nova transmissão. Neste caso, não importa o dado que existia
antes. Fazemos então a sua indicação como “don’t care”.
g) Tristate
Este
símbolo é usado para representar períodos de tempo nos=
quais um sinal digital encontra-se em tristate
(terceiro estado, ou alta impedância).
C=
omo
exercício você poderá agora fazer o download
de manuais de chips, memórias e processadores, encontrados nos sites=
dos
seus fabricantes, e observar os diagramas de tempo mostrados. Poderá
então entender melhor o funcionamento de vários desses chips.=
Ao
longo deste livro usamos vários diagramas de tempo para explicar o
funcionamento dos circuitos de um PC.
OBS: Quando um sinal tem valor 1
quando está em repouso e valor 0 quando está ativo, dizemos q=
ue
é um sinal de lógica negativa. Sinais com esta
característica são indicados com um traço horizontal s=
obre
o seu nome, ou então com um símbolo “#” à =
sua
direita, ou um “n” à sua esquerda. Por exemplo, se um si=
nal
RESET é ativo em 0, indicamos como RESET#=
ou nRESET.
Microel=
etrônica
A
microeletrônica consiste em projetar e produzir circuitos utilizando
componentes de tamanho microscópico. Usando mat=
erias
e técnicas apropriadas, é possível contruir
transistores, resistores, capacitores, diodos e indutores, cada um deles com
tamanhos menores que 1 milésimo de milímetro. Os componentes
tradicionais, comprados em forma avulsa no comércio e usados nos cir=
cuitos
de som, rádio e TV, são chamados de componentes discretos<=
/i>.
Um circuito integrado ou chip é um circuito complexo porém de tamanho reduzido. É equivalent=
e ao
circuito de uma placa com componentes discretos, mas pelo fato de utilizar
componentes integrados microscópicos, seu tamanho total é da
ordem de 1
centímetro quadrado, ou mesmo menor.
Os
componentes de um chip são como se fossem “pintados” na =
sua
minúscula base, chamada substrato. O seu processo de
fabricação é entretanto bem=
mais
complexo que uma simples pintura. Trata-se de um processo um pouco
químico, um pouco fotográfico, uma difusão de
moléculas dentro da base de silício, formando camadas que
compõem os circuitos.
A=
maioria
dos materiais são divididos em duas categ=
orias:
condutores e isolantes. O condutor é um material que t=
em
facilidade em conduzir corrente elétrica. Todos os metais são
condutores. Já os isolantes são materiais que dificultam a
passagem da corrente elétrica. A borracha é um exemplo
típico de isolante, assim como o vidro, madeira, plásticos em
geral, etc. Existem entretanto alguns materiais =
que
ora se comportam como condutores, ora como isolantes. São os chamado=
s semicondutores,
e os principais deles são o silício e o germânio.
A maioria dos transistores e chips utilizam o
silício em sua fabricação. O germânio é
utilizado em alguns componentes especiais, como transistores para altas
freqüências.
P=
ara que
os semicondutores possam variar sua resistividade, é preciso que lhe
sejam adicionados materiais especiais, chamados de dopagem. Existem
dopagens tipos N e P (negativa e positiva), e a sua combinação
é usada na formação dos transistores, diodos e demais
circuitos no interior de um chip.
|
|
Figura
3.51
Foto
ampliada do corte transversal de um microscópico trecho de um chip=
. A
parte mostrada mede alguns poucos milésimos de milímetro.
|
U=
m chip
é formado por sucessivas camadas de materiais diferentes. A base na =
qual
um chip é construído (substrato) é feita de silí=
;cio
puro, ou seja, sem dopagem. Sobre esta base são aplicadas dopagens
sucessivas, formando trechos tipos N e P. Eventuais ligações
são feitas com camadas de alumínio ou cobre. Em certos trechos
também são usadas camadas de óxidos como isolantes. &n=
bsp;
|
|
Figura
3.52
Funcionamento
de um transistor MOS e seu símbolo.
|
A=
figura
52 ilustra o funcionamento de um tipo especial de transistor usado para for=
mar
os chips. Trata-se do transistor MOS. Recebe este nome porque é form=
ado
por camadas de metal, óxido e semicondutor (Metal Oxide Semiconductor). Este transitor
possui três terminais, chamados de source=
,
drain e gate=
.
O terminal source é ligado à
tensão positiva da fonte, através de um resistor. Ele é=
; a
saída do circuito, que pode representar bits 0
ou 1. O terminal drain é ligado ao terra=
, ou
seja, o polo negativo da bateria. O terminal de
entrada é o gate, e é usado para
controlar a corrente que passa entre source e <=
span
class=3DSpellE>drain.
Q=
uando o gate é ligado a uma tensão baixa (bit 0=
),
não passa corrente entre source e drain. Sendo assim, o source
terá uma tensão elevada (bit 1), já que fica ligado ao=
polo positivo da bateria, através de um resist=
or.
Quando o gate é ligado a uma tensã=
;o
alta (bit 1), passará uma corrente entre source=
e drain. A resistência entre esses dois p=
ontos
será baixa, e a tensão medida no source<=
/span>
será próxima de 0 volt. Teremos assim um bit 0 em sua
saída. O circuito formado por este transistor e um resistor é=
o
que chamamos de inversor, e é mostrado na figura 53. A operaç&a=
tilde;o
lógica que realiza é a inversão de bits. Ao ser aplica=
do
um bit 1 na sua entrada, produzirá um bit 0 na saída. Ao ser
aplicado um bit 0 na entrada, produzirá um bit 1 na saída. &n=
bsp;
|
|
Figura
3.53
Inversor
MOS.
|
U=
m fator
bastante importante é a medida dos microscópicos transistores=
que
formam os chips, como os mostrados na figura 52. Com o passar dos anos,
dimensões cada vez menores têm sido utilizadas. A unidade usada
para medir esses transistores é o mícron (símbolo =
m). Cada mícron &eacut=
e;
equivalente a um milésimo de milímetro. Os chips modernos
apresentam transistores medindo uma fração do mícron. =
No
ano 2001, os processadores modernos usavam tecnologia de 0,18
mícron, e já existiam modelos com a tecnologia de 0,13
mícron. Usar transitores menores signifi=
ca:
· =
Menor
voltagem
· =
Menor
dissipação de calor
· =
Menor
custo de produção
A=
tabela
que se segue mostra a evolução das tecnologias de
fabricação nos últimos anos:
|
Ano
|
Tecnologia
|
Voltagem
|
|
1989
|
1 m
|
5
V
|
|
1991
|
0,8
m
|
5
V
|
|
1993
|
0,5
m
|
3,3
V
|
|
1995
|
0,35
m
|
2,5
V
|
|
1997
|
0,25
m
|
1,8
V
|
|
1999
|
0,18
m
|
1,5
V
|
|
2001
|
0,13
m
|
1,3
V
|
&=
nbsp;
|
|
Figura
3.54
Foto
ampliada de um transistor com 0,13m.
|
N=
ão
apenas transistores podem ser construídos através de
microeletrônica. Pequenos trechos de semicondutores podem formar
resistores. Placas paralelas de metal formam capacitores, e trilhas de metal
dispostas em forma espiral formam bobinas. Chips usados em telecomunica&cce=
dil;ões
utilizam no seu interior, bobinas e capacitores, além dos transistor=
es e
resistores. Chips usados em eletrônica digital (processadores,
memórias, chipsets, etc)
em geral apresentam apenas transistores e alguns resistores. A figura 55 mo=
stra
o trecho ampliado de um chip usado em telecomunicações, onde
podemos ver as espirais que formam as bobinas e as grandes áreas que
formam os capacitores.
|
|
Figura
3.55
Foto
ampliada do interior de um chip contendo bobinas e capacitores.
|
O=
s chips
são produzidos em grandes pastilhas circulares de 20 ou 30 cm de diâmet=
ro
chamadas waffers. A indústria tem
trabalhado durante os últimos anos com waffers<=
/span>
de 20 cm,
e apenas em 2001 começaram a ser adotados os wa=
ffers
de 30 cm,
com várias vantagens. Em cada waffer
são construídas dezenas ou centenas de chips, como vemos na
figura 56. Depois de prontos os chips são separados um dos outros
através de corte. São testados e finalmente encapsulados. &nb=
sp;
|
|
Figura
3.56
Vários
chips em um waffer.
|
O
processo de encapsulamento consiste em a=
lojar
a pastilha do chip em uma carcaça externa, que pode ser de plástico ou cerâmica. Também &e=
acute;
feita a ligação dos seus pontos de contato nos terminais exte=
rnos
(as “perninhas” do chip).
CMOS
Os
circuitos integrados digitais devem ter o menor número possív=
el
de resistores. Esses componentes, mesmo no interior dos chips, ocupam
áreas muito maiores que os transistores. Al&eacu=
te;m
disso produzem maior dissipação de calor e retardos que
tornam os chips mais lentos. Por isso os projetistas tentam na medida do
possível usar os próprios transistores para substituir os res=
istores.
Daí surgiram os circuitos CMOS (Complementary Metal Oxide Semico=
nductor).
Consiste em utilizar no circuito da figura 53, um segundo transistor no lug=
ar
do resistor. Este segundo transistor possui características inversas
às do primeiro. São chamados transistores complementares.
Um transistor é do tipo NMOS, e o outro é tipo PMOS. Quando um
transistor conduz, o outro não conduz, e vice-versa. O resultado
é o mesmo obtido com o uso do resistor, porém ocupando muito
menos espaço, consumindo menos energia e com mais velocidade. O arra=
njo
completo é mostrado na figura 57.
|
|
Figura
3.57
Circuito
equivalente de uma célula CMOS.
|
E=
ste
circuito é o inversor, o mais simples dos operadores
lógicos. Ele gera um bit 1 quando recebe um bit 0, e gera um bit 0
quando recebe um bit 1. Outras funções lógicas mais
complexas são implementadas com arranjos parecidos. Observe que ambo=
s os
transitores possuem seus terminais gate interligados. Quando esta entrada recebe =
um bit
1, ou seja, um nível de tensão elevado, o transitor
inferior conduzirá corrente, e o superior ficará cortado,
ou seja, sem conduzir. Isto fará com que a saída fique com
tensão baixa, ou seja, um bit 0. Quando a entrada receber um bit 0, o
transistor inferior ficará cortado, sem conduzir, e o transistor
superior irá conduzir, fazendo com que sua saída fique com uma
tensão quase igual à da fonte de alimentação (b=
it
1). A figura 58 mostra como o par CMOS é construído em um chi=
p.
|
|
Figura
3.58
Camadas
que formam o par CMOS.
|
A maioria dos chips modernos utilizam a tecnologia CMOS. Existem =
outras
tecnologias que são utilizadas em aplicações nas quais o CMOS não pode ser aplicado. Por exemplo=
, os
pares CMOS não são indicados quando é necessário
fornecer correntes elevadas, como por exemplo, para alimentar os slots de um barramento. N=
esses
casos são usados circuitos lógicos TTL, que consomem mais
energia, mas também podem fornecer mais corrente. Muitos chips utili=
zam
internamente células CMOS e externamente apresentam entradas e
saídas TTL.
M=
uitas
pessoas ouvem falar em CMOS pela primeira vez ao tomarem contato com o cham=
ado CMOS
Setup de placas de CPU. Acabam conhecendo o=
”chip
CMOS”, no qual existe uma pequena área de memória p=
ara
armazenar configurações do BIOS da placa de CPU, além =
de
um relógio permanente. O “chip CMOS” é alimentado=
por
uma bateria que o mantém em funcionamento mesmo quando o computador
está desligado. Aqui está um fato curioso: praticamente todos=
os
chips do computador utilizam a tecnologia CMOS.
É errado pensar que apenas o popular “chip CMOS” que
armazena os dados do Setup e tem o relóg=
io
permanente utiliza esta tecnologia.
Circuit=
os
lógicos
T=
oda a
eletrônica digital é desenvolvida a partir da
criação de circuitos capazes de executar operaç&oti=
lde;es
lógicas, também chamadas de operações booleanas. Os três principais operadores
lógicos são:
· =
E (AND)
· =
Ou
(OR)
· =
Não
(NOT)
A=
partir
desses operadores, circuitos ainda mais complexos são
construídos:
· =
Somadores
e Subtratores
· =
Multiplicadores
e divisores
· =
Células
de memória
· =
Registradores,
multiplexadores, decodificadores
· =
etc.=
..
A=
reunião
desses circuitos complexos forma chips bastante sofisticados, como
processadores, memórias, chips gráficos, chipsets,
etc. Parece incrível que equipamentos tão sofisticados possam=
ser
construídos a partir de circuitos básicos tão simples.=
Da
mesma forma como livros inteiros podem ser feitos a partir de letras e
símbolos, e como um planeta inteiro é construído a par=
tir
de prótons, elétrons, nêutrons e outras partícul=
as sub-atômicas.
Um
operador lógico é algo que lembra um pouco um operador
aritmético. Na aritmética temos operadores como
Adição, Subtração, etc. Da mesma forma como na
aritmética temos, por exemplo:
5=
+ 2 =3D 7
na
lógica temos
1=
AND 1 =3D
1
1 OR 0 =3D 1
NOT 1 =3D 0
I=
nicialmente,
vejamos como funcionam os três operadores citados. Eles podem ser def=
inidos
através da sua tabela verdade. A seguir temos essas tabelas:<=
span
class=3DGramE>
|
A
|
NOT A
|
|
A
|
B
|
A AND B <=
/b>
|
|
A
|
B
|
A OR B
|
|
0
|
1
|
|
0
|
0
|
0
|
|
0
|
0
|
0
|
|
1
|
0
|
|
0
|
1
|
0
|
|
0
|
1
|
1
|
|
|
|
|
1
|
0
|
0
|
|
1
|
0
|
1
|
|
|
|
|
1
|
1
|
1
|
|
1
|
1
|
1
|
C=
omo
vemos na tabela, o operador NOT, também chamado de inversor,
produz na sua saída o bit inverso daquele recebido na entrada. Ao
receber um bit 0, produz um bit 1 em sua saída. Ao receber um bit 1,
produz um bit 0. O operador AND possui duas entradas. Sua saída
será 1 quando as duas entradas também forem 1, simultaneament=
e.
Quando uma das suas entradas, ou ambas são 0, a
saída do operador AND será 0. Já o operador OR produz =
uma
saída 1 quando pelo menos uma das suas entradas tem o valor 1. Apenas
quando ambas as entradas são 0, o operador OR dará saí=
da
0.
&=
Eacute;
relativamente fácil produzir circuitos que realizam essas
funções, usando transistores, resitores<=
/span>
e outros componentes.
|
|
Figura
3.59
Inversor
RTL.
|
O
circuito mostrado na figura 59 implementa o operador lógico NOT.
É formado a partir de um transistor e dois resistores. Este
método de construção de circuitos é chamado RTL
(Resistor-Transistor Logic). Seu funcionamento
é bastante simples. Quando X é um bit 1, a tensão correpondente é um valor alto (porém me=
nor
que Vcc, a tensão da fonte de
alimentação). Este valor alto faz com que exista uma corrente=
na
base do transistor, que irá conduzir uma corrente elevada entre seus
outros terminais. Ao mesmo tempo aparecerá uma baixa tensão (=
da
ordem de 0,3 volts, dependendo do transistor) no seu coletor, que é a
saída Y. Temos então um bit 0 na saída. Da mesma forma,
quando X é um bit 0, a
tensão na entrada do transitor ser&aacut=
e;
baixa. O transitor ficará então
“cortado”, e praticamente não passará corrente por
ele. A tensão na saída Y dependerá apenas do resistor
ligado ao ponto Vcc. Teremos assim uma tens&ati=
lde;o
alta em Y, o que corresponde a um bit 1.
|
|
Figura
3.60
Circuito
OR RTL.
|
A=
figura
60 mostra como é implementado o operador OR usando a lógica R=
TL.
O primeiro transistor vai conduzir corrente quando pelo menos uma das duas
entradas, A ou B, estiver com tensão alta (bit 1), ficando assim com=
um
nível 0 no ponto X. Apenas quando ambas as entradas A e B estiverem =
em
0, o primeiro transistor ficará cortado e teremos um bit 1 no ponto =
X.
Ora, este é exatamente o inverso da função OR. Temos portanto no ponto X um outro operador lógico c=
hamado
NOR (ou NOT OR), cuja tabela verdade é:
|
A
|
B
|
A NOR B <=
/b>
|
|
0
|
0
|
1
|
|
0
|
1
|
0
|
|
1
|
0
|
0
|
|
1
|
1
|
0
|
P=
ara que
o circuito final tenha uma saída OR, e não NOR,
temos que usar mais um inversor, representado pelo segundo transisto=
r e
seus dois resistores.
A=
figura
61 mostra o circuito que implementa um operador lógico AND, usando a
técnica RTL. O primeiro estágio é formado por dois
transistores, sendo que cada um deles tem ligada na sua base, uma das entra=
das
(A ou B) do circuito. Para ter o valor 0 no ponto X é preciso que am=
bos
os transistores estejam conduzindo, o que é conseguido apenas quando
ambas as entradas A e B estão em 1. Se uma ou ambas as entradas esti=
ver
com o valor 0, o transistor correspondente estará cortado, e n&atild=
e;o
passará corrente através de ambos. Isto fará com que o
ponto X fique com o valor 1.
|
|
Figura
3.61
Circuito
AND RTL.
|
E=
sta
é exatamente o função inver=
sa do
AND, e é chamada NAND. Sua tabela verdade é:
|
A
|
B
|
A NAND B
|
|
0
|
0
|
1
|
|
0
|
1
|
1
|
|
1
|
0
|
1
|
|
1
|
1
|
0
|
P=
ara que
tenhamos na saída do circuito uma função AND, é
preciso inverter o sinal presente no ponto X, para isso utilizamos mais um
inversor, representado pelo terceiro transistor e seus resistores.
C=
ircuitos
lógicos como NOT, AND, OR, NAND, NOR e outros operadores, podem ser =
costruídos utilizando várias téc=
nicas.
Mostramos aqui o método RTL, porém existem outras formas de c=
riar
circuitos equivalentes, como:
DTL: Diode=
-Transistor
Logic
ECL: Emitter Couple=
d
Logic
TTL: Transistor-Transistor Logic
CMOS: Complementary Metal Oxide Semiconductor Logic
As
técnicas mais utilizadas são a TTL, para chips mais simples, e
CMOS para chips mais complexos.
Operado=
res
lógicos
Q=
uando
projetamos ou analisamos circuitos lógicos, não nos preocupam=
os
com detalhes internos, como seus transistores, diodos e resistores. Levamos=
em
conta apenas as entradas e saídas. Nos diagramas de circuitos digita=
is,
desenhamos apenas os símbolos dos circuitos que implementam as
funções lógicas. Chamamos esses circuitos de portas
lógicas. A figbura 62 mostra os
símbolos das principais portas lógicas.
|
|
Figura
3.62
Símbolos
das portas lógicas.
|
N=
esta
mesma figura apresentamos também as portas lógicas XOR (eXclusive OR – ̶=
0;ou
exclusivo”) e XNOR (eXclusive NOR). A
função XOR tem uma tabela verdade bastante parecida com a da
função OR. Seu significado é o seguinte: o bit de
saída será ligado se um dos bits de entrada estiver ligado, m=
as
não ambos ao mesmo tempo. Portanto a única diferença e=
ntre
as funções OR e XOR é que:
1 OR 1 =3D 1
1 XOR 1 =3D 0
|
A
|
B
|
A XOR B
|
|
A
|
B
|
A XNOR B
|
|
0
|
0
|
0
|
|
0
|
0
|
1
|
|
0
|
1
|
1
|
|
0
|
1
|
0
|
|
1
|
0
|
1
|
|
1
|
0
|
0
|
|
1
|
1
|
0
|
|
1
|
1
|
1
|
Motramos
também acima a tabela verdade do operador XNOR, que é o inver=
so
do operador XOR. Observe que a função XNOR funciona como um
comparador. Seu resultado é 1 quando os dois bits de entrada s&atild=
e;o
iguais, e 0 quando os dois bits de entrada são diferentes.
Circuit=
os
lógicos complexos
A
construção de circuitos lógicos complexos é uma
simples questão de agrupar essas portas básicas, produzindo
funções mais elaboradas. A figura 63, por exemplo, mostra o
circuito de um comparador binário. Este circuito faz a
comparação de dois valores binários de 4 bits cada um.=
A
saída do circuito será 1 quando os dois valores binári=
os
de 4 bits presentes nas entradas forem iguais. Digamos que esses valores se=
jam
representados por A3A2A1A0 e B<=
sub>3B2B1B0.
A saída Y do circuito será ativada em 1 quando tivermos iguais
esses valores. Por exemplo A=3D0110 e B=3D0110. =
Este tipo
de circuito é muito utilizado como decodificador de endereços=
nas
placas de CPU e nas placas de expansão. Os valores do endereç=
o A
podem ser originados no barramento de
endereços do processador, e os valores de B são originados em=
um
grupo de microchaves ou ju=
mpers,
que dependendo da forma como são configurados, podem indicar bits 0 =
ou
1. O circuito comparador irá ativar sua saída em 1 quando o
endereço recebido for igual ao endereço definido pelas microchaves ou jumpers.
Obviamente para isto é necessário um comparador maior, operan=
do
com maior númeor de bits, mas seu
princípio de funcionamento é o mesmo.
|
|
Figura
3.63
Comparador
de 4 bits.
|
U=
tilizando
um número maior de portas lógicas, podemos formar circuitos m=
ais
complexos. A figura 64 mostra o circuito de um contador binário de 4
bits. Este circuito recebe um sinal de clock e =
gera
nas suas 4 saídas, números binários na
seqüência 0000, 0001, 0010, etc. Pode ser programado para contar=
no
modo decimal, ou seja, passando de 9 (1001) para 0 (0000), ou então =
no
formato hexadecimal, passando de F (1111) para 0 (0000). Gera ainda um bit =
de
“vai 1”=
e pode ser agrupado com outros circuitos iguais, formando assim contadores =
com
qualquer número de dígitos. Pode ainda ser programado para fa=
zer
contagem crescente ou decrescente.
|
|
Figura
3.64
Contador
binário.
|
Um
projetista de hardware pode obter circuitos digitais de várias forma=
s. A
mais simples é utilizando chips padrões de mercado, que
normalmente apresentam encapsulamentos como os =
da
figura 65. Os encapsulamentos mostrados na figu=
ra
são o DIP (Dual In-Line Package)
e SOIC (Small Outline Integrated Circuit). Exis=
tem
circuitos com portas AND, OR, NOR, NAND, inversores, e funções
mais complexas mas de uso comum, como decodifica=
dores,
comparadores, contadores, registradores, etc.
|
|
Figura
3.65
Chips
com encapsulamento DIP plástico e SOIC=
.
|
N=
os
manuais dos chips que contém circuitos lógicos básicos,
encontramos diagramas que indicam o que existe no seu interior, como nos ex=
emplos
da figura 66. Os chips deste exemplo têm o seguinte conteúdo:<=
/span>
4=
portas
NAND de 2 entradas
3 portas AND de 3 entradas
4 portas AND de 2 entradas
2 portas NAND de 4 entradas
4 portas XOR de 2 entradas
1 porta NAND de 8 entradas
4 portas NOR de 2 entradas
4 portas OR de 2 enrtadas
6 inversores (portas NOT)
|
|
Figura
3.66
Diagramas
de alguns chips TTL.
|
Ao
projetar um circuito digital, usamos iniciamente as
portas necessárias para implemenetar a função desejada. Depois contamos quant=
as
portas de cada tipo são necessárias. Finalmente escolhemos os
chips apropriados que contenham as portas desejadas, e finalmente realizamo=
s as
ligações entre os pinos desses chips.
|
|
Figura
3.67
Diagrama
interno do chip 74LS181 – unidade lógica e aritmética=
de
4 bits.
|
A=
figura
67 mostra o diagrama interno do chip 74LS181. Este chip é uma unidade
lógica e aritmética de 4 bits, capaz de realizar 16
operações lógicas e aritméticas, entre
adição, subtração, AND, OR, etc. Vários
chips desses podem ser ligados em cascata para formar unidades com maior
número de bits. Este chip tem pouco mais de 60 portas lógicas=
. Em
um microprocessador existem vários milhões de portas
lógicas, executando entre outras, funções como as deste
chip, porém com maior número de bits. Como este capítu=
lo
destina-se apenas a dar noções sobre eletrônica, n&atil=
de;o
vamos analisar o funcionamento do circuito, mas acredite, ele realmente som=
a,
subtrai e faz várias outras
operações. Desta forma podemos entender como as portas
lógicas podem ser interligadas para formar um computador.
Como
construir uma memória com portas lógicas
P=
ara
construir um computador, não basta utilizar operadores lógico=
s e
aritméticos. É preciso também ter memória, uma
característica fundamental dos circuitos digitais. Células de
memória podem ser facilmente construídas a partir do diagrama
básico mostrado na figura 68. Este circuito é chamado de FLIP
FLOP.
|
|
Figura
3.68
Célula
de memória.
|
S=
uas duas
entradas R e S devem permanecer com valores 1. Para armazenar um bit 1 na
célula, basta aplicar momentaneamente um bit 0 na entrada S (Set). P=
ara
armazenar um bit 0 na célula, basta aplicar momentaneamente um bit 0=
na
entrada R (Reset). Vejamos como isto ocorre, de=
talhadamente.
a)
Suponha que as entradas estejam em repouso, ou seja, R=3D1 e S=3D1.<=
/p>
b)
Aplicamos momentaneamente um bit 0 em
S. A porta NAND ligada em S, ao receber 0 nesta entrada,
produzirá uma saída Y=3D1 (lembre-se da tabela verdade da
função NAND: se pelo menos uma das entradas é 0, a saída &eac=
ute; 1).
c=
) A
porta 2 está então recebendo as entradas R=3D1 e Y=3D1 (note =
que a
saída Y do circuito funciona como entrada da porta 2). Como 1 NAND 1=
=3D
0, teremos uma saída X=3D0 na saída da porta 2. Este zero, ao
entrar na porta 1, continuará produzindo saída Y=3D1, e agora=
isto
independe do valor de S, já que 0 NAND 0 =3D 1 e 0 NAND 1 =3D1.
d=
) Agora
a entrada S pode voltar ao seu valor de repouso 1, e a saída Y
continuará sendo mantida em 1. Temos então um bit 1 armazenad=
o.
D=
a mesma
forma, o circuito também pode armazenar um bit 0, bastando manter S =
em
1, e momentaneamente levando a entrada R ao valor 0. O que ocorre é o
seguinte:
a=
) Ao
receber uma entrada 0 em R, a porta 2 produzirá uma saída X=
=3D1. A
porta 1 está recebendo neste momento, X=3D1 e S=3D1. Portanto temos =
Y =3D 1
NAND 1, que vale 0.
b=
) O
valor Y=3D0 chega à entrada da porta 2. Como 0 NAND (qualquer coisa)=
vale
1, teremos X=3D1, independentemente do valor de R, que agora pode voltar ao=
seu
estado de respouso, ou seja, com valor 1.
c=
) A
porta 1 está recebendo as entradas X=3D1 e S=3D1. Como 1 NAND 1 =3D =
0, mais
uma vez temos reforçado o bit 0 na saída Y.
d=
) As
entradas R e S podem voltar aos seus valores de repouso (R=3D1 e S=3D1) e o
circuito manterá armazenado um bit Y=3D0.
&=
Eacute;
um circuito extremamente simples, mas é realmente uma surpresa a sua
capacidade de “lembrar” um bit. Circuitos como este
são agrupados até formar células de memó=
ria
com muitos bits. Milhões dessas células são encontradas em um chip de memória, formando
vários megabytes.
Projetando chips
O
método mais simples para projetar circuitos lógicos é
utilizar chips básicos como os mostrados na figura 66. Este é=
um
método indicado para a construção de protótipos=
ou
projetos de pequena complexidade. Para produção profissional<=
span
class=3DGramE> entretanto, é preciso utilizar métodos =
mais
eficientes.
C=
ircuitos
lógicos de média complexidade tornam-se muito grandes quando
utilizamos chips básicos. Uma solução para esses casos
é utilizar microcontroladores. Esses chi=
ps
são microprocessadores que possuem em seu interior, uma unidade de
processamento, memória ROM, RAM e circuitos de apoio. Quando o circu=
ito
a ser projetado não precisa ser extremamente veloz (por exemplo, uma
placa lógica para controlar uma máquina de refrigerantes, ou
máquina de lavar, ou o painel de controle de um videocassete), a mel=
hor
solução não é construir um circuito, e sim um
programa que receba as entradas e gere as saídas. Quando o circuito a
ser criado precisa ser muito veloz, os microcontroladores tornam-se ineficientes. Uma
solução bastante viável é utilizar chips
programáveis. Esses chips possuem em seu interior, um grande
número de portas lógicas. Através de um programa de CA=
D,
criamos o circuito com o auxílio de um PC e simulamos o seu
funcionamento. Terminado o projeto, o circuito é “gravado̶=
1;
no chip programável. Esta programação consiste em defi=
nir
as conexões que são realizadas entre os módulos intern=
os
do chip programável. Tais chips programáveis são chama=
dos
de PLD (programmable logic=
devices) e EPLD (eraseable programmable logic devices). Os dois principais fabricantes desses produ=
tos
são a Altera (www.altera.com) =
e Xilinx (www.xilinx.=
com).
U=
tilizando
PLDs e EPLDs,
projetos complexos podem ser criados em pouco tempo, e ficam extremamente
compactos. Até mesmo a produção em série pode s=
er
feita, em pequena escala. Quando a escala de produção é
maior e os custos finais do produto precisam ser reduzidos, a melhor coisa a
fazer é projetar chips novos.
O=
projeto
de chips é feito através de programas especiais de CAD. Defin=
imos
os circuitos lógicos a serem utilizados e simulamos o funcionamento =
do
circuito final, tudo através de um PC. Terminado o projeto, o progra=
ma
de CAD irá gerar arquivos de impressão, que transferidos para=
um
equipamento apropriado, irão resultar em fotolitos. Esses
fotolitos são levadas a uma máquina de produção=
de
chips, que podem então ser produzidos aos
milhares, com baixo custo unitário de produção. Todo e=
ste
equipamento é muito caro, e até mesmo a contrataç&atil=
de;o
de empresas especializadas tem custo elevado, e só compensa quando os
chips são produzidos aos milhares.
Convers=
ores
D/A e A/D
N=
em
só com circuitos digitais se faz um computador. Também s&atil=
de;o
necessários os circuitos analógicos. Sua função
básica é lidar com sinais analógicos. Os principais
circuitos analógicos são os existentes na placa de som, no mo=
dem
e o trecho da placa de vídeo que envia as informações =
de
cor para o monitor. Circuitos analógicos são formados por transitores, resistores, capacitores, indutores, diod=
os,
transformadores e outros componentes “não digitais”. Para
exemplificar esses circuitos, mostraremos aqui o funcionamento dos converso=
res
D/A (Digital-Analógicos) e A/D (Analógicos-Digitais).
Os conversosres D/A são encontrados na p=
laca
de som, fazendo a conversão de sons digitalizados para o formato
analógico, podendo assim ser amplificados e enviados para os alto
falantes. Esses circuitos também são utilizados na placa de
vídeo. Os dados existentes na memória de vídeo s&atild=
e;o
digitais, e passam por conversores D/A para que se transformem em sinais
analógicos, transmitindo informações sobre a quantidad=
e de
vermelho, verde e azul em cada pixel da tela.
A=
base do
funcionamento dos conversores D/A e A/D é um circuito chamado amp=
lificador
operacional. Ligado convenientemente em capacitores, resistores e diodo=
s,
este circuito é capaz de realizar várias operaçõ=
;es
matemáticas sobre sinais analógicos. Pode até mesmo ser
usado para sintetizar sons similares aos dos instrumentos musicais. Os
amplificadores operacionais são fabricados com =
encapsulamentos
similares aos dos chips e transistores.
|
|
Figura
3.69
Circuito
básico com amplificador operacional.
|
A=
figura
69 mostra uma das formas mais simples de uso de um amplificador operacional.
Possui duas entradas analógicas e uma saída. A tensão =
de
saída Vo é igual à tens&at=
ilde;o
existente entre suas duas entradas, multiplicada por um fator de
amplificação, que é bastante grande, em geral superior=
a
1000. No circuito da figura, uma das entradas está ligada no terra (0 volts), e a outra entrada tem o valor de
tensão Vx. Chamamos o ganho do amplifica=
dor de
A (lembre-se que o ganho do amplificador é muito grande). Entã=
;o
temos:
Vo =3D
A.Vx
Vx =3D Vo/A
C=
omo A
é um valor muito grande, é correto dizer que Vx
é um valor muito pequeno. Na prática é de apenas alguns
milésimos de volts, e é correto, para efeito de cálcul=
os
aproximados, considerar Vx<=
/span>=3D0.
Tomando Vx=3D0, as correntes i1 e i2 que chegam=
ao
ponto X são:
i1 =3D Va/Ra
i2 =3D Vo/Ro
A corrente i que “entra” no amplificador é igual à s=
oma
de i1 e i2
i =3D
i1 + i2
U=
ma outra
característica dos amplificadores operacionais é que sua
resistência de entrada é elevadíssima, da ordem de algu=
ns
milhões de ohms. Isto é o mesmo que dizer que sua corrente de
entrada é muito pequena, praticamente zero. Portanto podemos conside=
rar
que i=3D0.
i =3D
i1 + i2 =3D 0, ou seja
i2 =3D
-i1
S=
ubstituindo
i1 por Va/Ra e i2 p=
or Vo/Ro, ficamos com:
Vo/Ro =3D - Va/Ra
Vo =3D - Va (Ro/Ra<=
/span>)
C=
oncluímos
então que a tensão de saída Vo
é igual à tensão de entrada Va,
multiplicada por um fator de amplificação Ro/Ra,
com sinal negativo. Por exemplo, se fizermos Ro =3D 10k=
W e Ra=3D
1kW,
teremos Vo =3D -10.<=
span
class=3DSpellE>Va. Conseguiríamos assim um circuito cuja
saída é sempre 10 vezes maior que a entrada, com sinal negati=
vo.
Este sinal negativo pode, caso seja necessário, ser eliminado por um
segundo estágio com ganho igual a –1, conseguido fazendo Ro=3D=
Ra.
|
|
Figura
3.70
Amplificador
com duas tensões de entrada.
|
O
circuito da figura 70 é um pouco mais complexo. Ele tem duas entrada=
s Va e Vb, com dois resisto=
res
correspondentes, Ra e Rb.
Nesses resistores passam correntes ia =3D Va/Ra e ib =3D Vb/Rb.
A corrente i1 neste caso vale ia+ib. A corrente i2 é Vo/Ro,
como no exemplo anterior, e a corrente i de entrada no amplificador operaci=
onal
vale aproximadamente zero. Temos então:
0=
=3D i =3D Vo/Ro + Va/Ra
+ Vb/Rb, ou seja:
Vo =3D - (Va.Ro/Ra<=
/span> + Vb.Ro/Rb) =3D -Ro(Va/Ra
+ Vb/Rb)
|
|
Figura
3.71
Amplificador
com múltiplas entradas analógicas. Um conversor D/A é
formado com este circuito, através da escolha apropriada dos
resistores.
|
E=
ste
resultado pode ser generalizado no circuito da figura 71, onde temos n entr=
ada
com tensões V1, V2,... Vn, e resistores =
R1, R2, ..., Rn:
Vo =3D
- Ro(V1/R1 + V2/R2 + V3/R3 + .... + Vn/Rn)
E=
ste
circuito pode ser usado como um conversor analógico digital. Suponha=
que
sua entrada seja formada por 4 bits. Digamos que=
os
valores de tensão correspondentes aos bits 0 e
1 sejam 0 volts e 1 volt, respectivamente. Tomemos para os resistores, os
seguintes valores:
R=
o =3D 8kW
R=
1 =3D 8kW
R=
2 =3D 4kW
R=
3 =3D 2kW
R=
4 =3D 1kW
F=
icamos
então com:
Vo =3D
-8000 (V1/8000 + V2/4000 + V3/2000 + V4/1000), ou seja:
Vo =3D
- (V1 + 2.V2 + 4.V3 + 8.V4)
N=
ote que
com este circuito, os valores de tensão (que correspondem aos bits do
valor digital de entrada) aparecem com pesos 1, 2, 4 e =
8,
exatamente como no sistema binário. Se tivermos =
por
exemplo as entradas V4V3V2V1 representando o valor binário 01=
10
(6 em decimal), ficamos com:
Vo =3D
- (1.0 + 2.1 + 4.1 + 8.0) =3D - 6 volts
P=
ortanto
o valor digital 6 (0110) gerou na saída do
circuito, o valor analógico de –6 volts. Da mesma forma o valor
digital 5 (0101) resulta no valor analógi=
co de
–5 volts, o valor digital 11 (1011) resulta no valor analógico
igual a –11 volts, e assim por diante. Nosso circuito é um
conversor digital-analógico de 4 bits.
C=
onversores
D/A com maior número de bits são construídos de forma
semelhante, bastando usar um maior número de entradas, com resistores
formando uma progressão geométrica de razão 2, ou seja, cada resistor é o dobro do anterior.
Placas de som utilizam conversores D/A de 8 e 16=
bits.
Placas de vídeo usam conversores D/A de 8=
bits,
gerando assim 256 tonalidades para cada componente de cor.
Um
conversor D/A precisa funcionar de forma tão rápida quanto os
sinais analógicos que precisa representar. Conversores D/A usados em
placas de som operam com 8 ou 16 bits, e usam ta=
xas de
amostragem de até 44 kHz, ou seja, fazem 44.000 conversões por
segundo. Conversores D/A usados em placas de vídeo operam com 8 bits e usam taxas de amostragem bem mais elevadas,
chegando a ultrapassar a casa dos 100 MHz, ou seja, acima de 100 milh&otild=
e;es
de conversões por segundo.
A
conversão A/D (de analógico para digital) é bem mais
complexa. Encontramos esses conversores em placas de som e placas
digitalizadoras de vídeo.
|
|
Figura
3.72
Conversor
Analógico/Digital.
|
A=
figura
72 mostra o funcionamento de um conversor Analógico/Digital. É
composto de um contador binário, um comparador analógico e um
conversor D/A. O valor analógico Vi &eacu=
te;
alimentado na entrada do conversor. Um sinal digital START dá
início à contagem realizada pelo contador binário. O v=
alor
binário gerado por este contador é enviado a um conversor D/A=
. O
valor analógico resultante desta contagem é comparado com o v=
alor
analógico Vi que está sendo convertido. No instante em que o
comparador detecta que suas entradas são iguais, significa que o val=
or
binário gerado pelo contador é a versão digital do val=
or
analógico Vi. Este comparador envia um sinal de parada ao contador. O
valor digitalizado pode então ser lido das saídas do contador
digital.
O
processo de conversão A/D é bem mais lento que o de
conversão D/A, e a sua rapidez depende de como é feita a contagem. Por exemplo, se usarmos um contador de 8 bits e for feita uma contagem seqüencial (0, 1,=
2, 3,
...), a conversão poderá demorar até 256 ciclos. Com u=
ma
contagem seqüencial em um conversor de 16 bits, esta conversão
poderá demorar até 65.536 ciclos. Para tornar a convers&atild=
e;o
mais rápida, os contadores utilizados não fazem contagem
seqüencial, e sim, realizam o que chamamos de “busca
binária”. Ao invés de contarem a partir do bit menos
significativo, começam a contar a partir do bit mais significativo. =
Ao
ligar o bit mais significativo, o valor analógico gerado será
igual ao ponto médio da escala de contagem (por exemplo, 128, em um
contador de 8 bits, que conta de 0 a 256). Se o valor as=
sim
gerado for muito grande, este bit será desligado. Se for menor que a
tensão procurada, este bit será mantido ligado. A seguir &eac=
ute;
feito o mesmo teste com o segundo bit mais significativo (em um contador de=
8 bits, ele tem peso 64), depois com o próximo =
(peso
32), e assim por diante, até chegar ao bit menos significativo. Desta
forma um conversor A/D de 8 bits realiza a
conversão em apenas 8 ciclos ao invés de 256. Um conversor A/=
D de
16 bits fará a conversão em 16 ciclos, ao invés de 65.=
536.
A rapidez da conversão depende portanto da
eficiência do método de contagem binária.
C=
onversores
A/D usados em placas de som operam com a mesma velocidade dos seus converso=
res
D/A, ou seja, até 44 kHz (44.000
conversões por segundo). Os conversores usados em placas digitalizad=
oras
de vídeo trabalham com 8 bits e
freqüências da ordem de 10 MHz, ou seja, fazem cerca de 10
milhões de conversões por segundo.
Fonte de
alimentação linear
A=
fonte
de alimentação é um dispositivo que tem a mesma
função que uma bateria. A diferença é que a ene=
rgia
elétrica não fica armazenada em células de voltagem (c=
omo
ocorre com pilhas e baterias), e sim, é extraída da rede
elétrica. Muitos aparelhos são alimentados diretamente a part=
ir
da rede elétrica, como é o caso de lâmpadas e motores. A
voltagem da rede elétrica não é adequada para aparelhos
eletrônicos, portanto esses aparelhos possuem fontes de
alimentação. São circuitos que convertem a tensã=
;o
da rede elétrica (110 volts em corrente alternada) para tensõ=
es
adequadas ao seu funcionamento (em geral inferiores a 20 volts, em corrente
contínua).
|
|
Figura
3.73
Tensão
contínua e tensão alternada.
|
A=
figura
73 mostra a diferença entre uma fonte de tensão contín=
ua e
uma alternada. Na fonte de tensão contínua (CC), a corrente
trafega sempre no mesmo sentido. O valor da tensão é constant=
e, e
se ligarmos um circuito de características constantes, como
lâmpadas e resistores, a corrente também será constante.
Como já mostramos, existem dois terminais, o positivo e o negativo. =
Na
fonte de corrente alternada (CA), a corrente trafega, ora em um sentido, or=
a em
outro sentido. A fonte CA empurra e puxa a corrente, indefinidamente.
A=
rede
elétrica usada no Brasil opera com 60 ciclos por segundo, ou seja,
empurra a corrente, depois puxa a corrente, e repete este ciclo 60 vezes a =
cada
segundo. Dizemos que a tensão da rede é 60 Hz. Em alguns
países, sobretudo na Europa, a rede opera com 50 Hz. O gráfic=
o da
tensão alternada tem a forma de uma senó=
ide
porque a geração é feita por eixos rotativos, existent=
es
nos geradores das usinas de energia. Uma vantagem da tensão alternada
é que pode ser facilmente convertida em valores mais altos ou mais b=
aixos,
através de transformadores, coisa que não pode ser feita
tão facilmente com a corrente contínua.
U=
ma fonte
de alimentação recebe corrente alternada a partir da rede
elétrica, com freqüência de 60 Hz e voltagem que pode ser=
de
110 ou 220 volts. Inicialmente esta tensão é reduzida para um
valor menor, através de um transformador. Temos
então corrente alternada, mas com um valor menor. A seguir
é feita uma retificação, que consiste em fazer a corre=
nte
trafegar sempre no mesmo sentido. O próximo passo é a filtrag=
em,
e finalmente a regulação. A figura 74 mostra as etapas da
geração de tensão contínua em uma fonte.=
<=
!--[if gte vml 1]>
![](3D"eletronicabasica_arquivos/image073.jpg")
Figura
3.74 - Operação de uma fonte linear.
A=
s fontes
que operam como motramos na figura 74 sã=
o as
chamadas “fontes lineares”. Sua principal desvantagem é =
que
requerem transformadores muito pesados para fazer a redução de
voltagem, e capacitores muito grandes para fazer a filtragem. São
adequadas quando a potência a ser fornecida (potência =3D
tensão x corrente) é pequena. Os chamados “adaptadores
AC”, usados para alimentar caixas de som e dispositivos que não
possuem fonte própria, consomem pouca potência. Eles sã=
o na
verdade fontes lineares de alimentação, com
operação similar ao mostrado na figura 74.
Fonte de
alimentação chaveada
T=
anto os
transformadores quanto os capacitores usados nas fontes de
alimentação poderiam ser bem menores se a freqüênc=
ia
da rede elétrica fosse mais elevada, ao invés de operar com
apenas 60 Hz. Por isso foram criadas as fontes chaveadas, utilizadas nos PCs e em todos os equipame=
ntos
eletrônicos modernos. Elas não necessitam de tranformadores
e capacitores grandes, e por isso podem fornecer muita potência,
porém mantendo peso e tamanho reduzidos.
|
|
Figura
3.75
Operação
de uma fonte chaveada.
|
A=
figura
75 mostra as etapas de funcionamento de uma fonte chaveada. Inicialmente a
tensão da rede elétrica é retificada e filtrada.
Não existe dificuldade técnica na retificação de
tensões elevadas. Quanto à filtragem, podem ser usados
capacitores de menor valor, pois a corrente é mais baixa,
apesar da tensão ser elevada. O resultado é uma tensão
contínua de valor elevado. Esta tensão passa por um transisto=
r de
chaveamento que a transforma em uma onda quadrada de alta
freqüência, entre 100 e 200 kHz. Este
transistor opera como uma chave elétrica que abre e fecha o circuito=
para
a passagem de corrente, em alta velocidade. Esta onda quadrada passa por um
transformador e tem sua tensão reduzida, porém com valor de
corrente maior. Este transformador pode ser pequeno, já que opera com
freqüência muito mais elevada, e quanto maior é a
freqüência, maior é a facilidade que um transformador tem
para fazer o seu trabalho.
T=
emos
então uma corrente alternada, mas com amplitude menor e
freqüência maior. Esta corrente é
retificada e filtrada, desta vez usando capacitores de menor tamanho=
, já
que a filtragem também é facilitada pela freqüência
elevada. Finalmente temos a etapa de regulação, na qual
imperfeições são eliminadas, resultando em um valor
constante na saída. Uma fonte de alimentação usada em um PC possui v&aacut=
e;rias
seções para a geração dos diversos valores de
voltagem.
------=_NextPart_01C99F13.BFDF7EA0
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