lecture 13

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Lecture 13 Today we will Examine how the logic gate model (RC circuit) reacts to a sequence of input changes Relate these results to clocking speed Define propagation delay Introduce digital logic gates Examine how signals propagate through logic circuits

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Lecture 13. Today we will Examine how the logic gate model (RC circuit) reacts to a sequence of input changes Relate these results to clocking speed Define propagation delay Introduce digital logic gates Examine how signals propagate through logic circuits. Vin. Vin. Vout. Vout. time. - PowerPoint PPT Presentation

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Page 1: Lecture 13

Lecture 13

Today we will Examine how the logic gate model (RC circuit) reacts

to a sequence of input changes Relate these results to clocking speed Define propagation delay Introduce digital logic gates Examine how signals propagate through logic circuits

Page 2: Lecture 13

time

Vin

0

time

Vin

0

Vout

time

Vin

0

Vout

Sequential Switching

What if we step up the input to a logic circuit,

wait for the output to respond,

then bring the input back down to perform the next computation?

Page 3: Lecture 13

We need to wait for the output to reach a recognizable logic level, before changing the input again.

This affects clock speed.

Pulse Distortion

0

1

2

3

4

5

6

0 1 2 3 4 5Time

Vin,

Vo

ut

Pulse width = RC

+

Vout(t)

R

Vin(t) + C

0123456

0 5 10 15 20 25Time

Pulse width = 10RC

Vin,

Vo

ut

Page 4: Lecture 13

Example

Suppose that the capacitor is discharged at t=0.

With Vin(t) as shown, find Vout(t).

+

Vout(t)

Vin(t) + 1 nF

2.5 k

4 V

5 s

Vin(t)

t

Page 5: Lecture 13

Example

First, Vout(t) will approach 4 V exponentially. We write the equation for this part using:

Initial condition Vout(0) = 0 V

Final value Vout,f = 4 VTime constant RC = (2.5 k)(1 nF) = 2.5 s

Vout(t) = Vout,f + (Vout(0)-Vout,f)e-t/RC

Vout(t) = 4-4e-t/2.5s V for 0 ≤ t ≤ 5 s

Page 6: Lecture 13

Example

Then, at 5 s, Vout(t) will approach 0 V exponentially. We write the equation for this part using:

Initial condition Vout(5 s) = ?

Use equation from previous step, since Vout is continuous.

Vout(5s) = 4-4e-5s/2.5s = 3.44 V

Final value Vout,f = 0 V Time constant RC = (2.5 k)(1 nF) = 2.5 s

Vout(t) = Vout,f + (Vout(t0) -Vout,f)e-(t-t0)/RC

Vout(t) = 3.44e-(t-5s)/2.5s for t > 5 s

Page 7: Lecture 13

00.5

11.5

22.5

33.5

4

0 2 4 6 8 10

Vout(t) =4-4e-t/2.5s for 0 ≤ t ≤ 5 s

3.44e-(t-5s)/2.5s for t > 5 s{

Example

Vin(t)

Vout(t)

t (s)

Page 8: Lecture 13

Design Issues

How long between successive inputs?Need output to reach recognizable logic levelOutput must be at this level long enough to serve as

input to next logic gate How many consecutive logic gates does signal go

through before being “cleaned up” or saved in staticmemory cell?Eventually the signal gets really badBut adding hardware adds cost and delay

Page 9: Lecture 13

Propagation Delay

Suppose an input goes from some initial voltage to some final voltage.

In our examples, the input switch is immediate, but in practice it is not.

Propagation delay is officially defined as:

(time when output is halfway to final value) minus

(time when input is halfway to final value)

Page 10: Lecture 13

Illustration

Using our equation for Vout(t), we can find:

tP,LH

(time when Vout(t) = 2 V, as it goes from 0 V to 4 V) – 0 s

tP,HL

(time when Vout(t) = 1.72 V, as it goes from 3.44 V to 0 V) – 5 s

00.5

11.5

22.5

33.5

4

0 2 4 6 8 10

tP,HL

tP,LH

tP,HL = tP,LH = 1.725 s

Page 11: Lecture 13

Propagation Delay

It’s not a coincidence that the propagation delays were the same.

For a general RC circuit that has an input voltage switch at t = t0,

Vout(t) = Vout,f + (Vout(t0) -Vout,f)e-(t-t0)/RC

The time when Vout(t) is ½ (Vout,f + Vout(t0)) is given by

½ (Vout,f + Vout(t0)) = Vout,f + (Vout(t0) -Vout,f)e-(t-t0)/RC

Simplifying,

½ = e-(t-t0)/RC t = (ln 2)(RC) + t0

The propagation delay, the difference between this time and t0, is

tP = (ln 2)(RC) Depends only on time constant!

Page 12: Lecture 13

Graphing Propagation through Multiple Logic Gates

We will want to examine how these RC-related delays affect a signal going through multiple logic gates.

The math involved in putting an RC output (decaying exponential) into another RC circuit is not so easy.

So, when analyzing a circuit with many logic gates, we will use the following simplification:

Logic Gate0 t

V

tPt

V

→ →

Page 13: Lecture 13

Logic Gates

We have been using a simple RC circuit to model a logic gate.

In each case, the final value of Vout was Vin.

This will not always be true; sometimes, the output will go to logic 0 when the input is logic 1 and vice-versa.

To determine what the final value of a logic gate output will be, we need to learn the types of logic gates.

Page 14: Lecture 13

Logic Gates

A

BC=A·BAND C =

A

BNAND BA

NORA

BBA

A A

ORA

BC=A+B

(EXCLUSIVE OR)

A

BBAC NOT XOR

Page 15: Lecture 13

Logic Functions: Truth Tables

We specify what a logic circuit does by listing the output for each possible input. This listing is called a truth table.

A A

0 1

1 0

NOT

A B A·B A·B

0 0 0 1

0 1 0 1

1 0 0 1

1 1 1 0

AND NAND

Page 16: Lecture 13

Logic Functions: Truth Tables

A B A+B A+B

0 0 0 1

0 1 1 0

1 0 1 0

1 1 1 0

OR NOR

A B A B A B0 0 0 1

0 1 1 0

1 0 1 0

1 1 0 1

XOR XNOR

Page 17: Lecture 13

Timing Diagrams

Now let’s look at how signals propagate through logic gates, taking delay into consideration.

Sketch the output for each logic gate in a more complicated circuit.

A

B

A(A)·B

t1

0

A, B

t1

0

A

tP

t1

0 tP

(A)·B

2tP

Invalid info!

Page 18: Lecture 13

Strategy for Timing Diagrams

To find the output for a particular gate,

Graph the inputs for that gate

Graph the result of the logic gate using the input graphs

Shift right by one tP

Page 19: Lecture 13

Example

D

AB

C

t1

0

A, B, C

Page 20: Lecture 13

Example

t

1

0

t

1

0

t

1

0

t

1

0

D

AB

C

tP

tP 2tP

tP

2tP 3tP

B A+C

(B)·C D