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NMOS & CMOS inverter and gates Unit II

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Page 1: VLSI_Design_-_Unit II - Part I

NMOS & CMOS inverter and gates

Unit II

Page 2: VLSI_Design_-_Unit II - Part I

NMOS & CMOS Digital Logic Inverter

S. B. Sivasubramaniyan MSEC, Chennai

Page 3: VLSI_Design_-_Unit II - Part I

CMOS Inverter

It is the basic building block of any digital system We had discussed the operation of the circuit

earlier

S. B. Sivasubramaniyan MSEC, Chennai

Page 4: VLSI_Design_-_Unit II - Part I

CMOS Inverter - Operation

S. B. Sivasubramaniyan MSEC, Chennai

Page 5: VLSI_Design_-_Unit II - Part I

CMOS Inverter – Operation

S. B. Sivasubramaniyan MSEC, Chennai

Page 6: VLSI_Design_-_Unit II - Part I

CMOS Inverter - inference

The output voltage levels are 0 and VDD. This shows the signal swing is maximum

The static power dissipation is zero A low resistance path exists between output and ground and

output and VDD The low resistance path is independent of W/L ration of the

transistor The input resistance is infinite. Thus the inverter can drive

large number of similar inverters but the delay rises accordingly

S. B. Sivasubramaniyan MSEC, Chennai

Page 7: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

Repetition of the above graphical procedure for intermediate values gives rise to voltage transfer characteristics

The current equations of the two transistors in the two regions of operation is given by

S. B. Sivasubramaniyan MSEC, Chennai

' 20

1

2

,

DN n I tn on

o I tn

Wi k v V v v

L

for v v V

2'1

2

,

DN n I tnn

o I tn

Wi k v V

L

for v v V

Page 8: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

The current equations of the two transistors in the two regions of operation is given by

S. B. Sivasubramaniyan MSEC, Chennai

2' 1

2

,

DP p DD I tp DD o DD op

o I tp

Wi k V v V V v V v

L

for v v V

2'1

2

,

DP p DD I tpp

o I tp

Wi k V v V

L

for v v V

Page 9: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

The CMOS inverter is usually designed to have the equal threshold voltage and

We know, The electron mobility is 2 to 2.5 times higher than that of holes

so to make

The width of the p-channel devices is made 2 to 2.5 times larger

Note: Both devices are designed to have equal Length

S. B. Sivasubramaniyan MSEC, Chennai

' 'n p

n p

W Wk k

L L

' '&n n ox p p oxk C k C

' 'n p

n p

W Wk k

L L

Page 10: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

The width of the two devices are related by

S. B. Sivasubramaniyan MSEC, Chennai

' 'n p

n p

W Wk k

L L

n ox p oxn p

W WC C

L L

n n p pW W n pL L

p n

n p

W

W

Page 11: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

When this is accomplished, we say that the CMOS inverter is symmetric

The Voltage transfer characteristic will be symmetric

S. B. Sivasubramaniyan MSEC, Chennai

Page 12: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

To determine VIH, we need to equate the current of QN and QP

QN operates in the triode region and QP operates in the saturation region

Equating the currents, we get

S. B. Sivasubramaniyan MSEC, Chennai

2 20

1 1

2 2DD I tn I tn oV v V v V v v

Page 13: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

Differentiate both sides relative to VI, and substitute

We get,

Substitute,

S. B. Sivasubramaniyan MSEC, Chennai

& 1oI IH

I

dvv V

dv

2DD

o IH

Vv V

&2DD

I IH o IH

Vv V v V

Page 14: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

We get,

Similarly

From VIL and VIH, we can determine Noise Margins

S. B. Sivasubramaniyan MSEC, Chennai

15 2

8IH DD tV V V

13 2

8IL DD tV V V

H OH IHNM V V

13 2

8H DD tNM V V

L IL OLNM V V

13 2

8L DD tNM V V

Page 15: VLSI_Design_-_Unit II - Part I

The Voltage Transfer Characteristics

Symmetrical transistors assumptions gave rise to identical noise margins

S. B. Sivasubramaniyan MSEC, Chennai

Page 16: VLSI_Design_-_Unit II - Part I

Problem

For a CMOS inverter with matched MOSFETs having Vt = 1 V, find

VIL , VIH and the noise margins if VDD = 5V

S. B. Sivasubramaniyan MSEC, Chennai

Page 17: VLSI_Design_-_Unit II - Part I

Solution

We know,

Substituting, we get

Similarly,

S. B. Sivasubramaniyan MSEC, Chennai

15 2

8IH DD tV V V

15 5 2 1

8IHV 2.875IHV V

13 2

8IL DD tV V V 13 5 2 1 2.125

8ILV V

Page 18: VLSI_Design_-_Unit II - Part I

Solution

We know,

Substituting, we get

Similarly,

S. B. Sivasubramaniyan MSEC, Chennai

13 2

8H DD tNM V V

13 5 2 1

8HNM 2.1HNM V

L HNM NM

Page 19: VLSI_Design_-_Unit II - Part I

Problem

Consider a CMOS inverter with , (W/L)n = 20, (W/L)p = 40, , and VDD = 10 V. For , find the maximum current that the inverter can sink while remains

S. B. Sivasubramaniyan MSEC, Chennai

2tn tpV V V 22 20 /n ox p oxC C A V

I DDv V0.5Vov

Page 20: VLSI_Design_-_Unit II - Part I

Solution

Sinking current is taken care by NMOS transistor For , NMOS transistor will operate in the

triode region (?) The current equation is given by

The maximum current for , will occur when

S. B. Sivasubramaniyan MSEC, Chennai

20

1

2tnDN n ox I on

Wi C v V v v

L

0.5ov V

0.5ov V

0.5ov V

Page 21: VLSI_Design_-_Unit II - Part I

Solution

Substituting, we get

S. B. Sivasubramaniyan MSEC, Chennai

20

1

2tnDN n ox I on

Wi C v V v v

L

2120 20 10 2 0.5 0.5

2DNi

1.55DNi mA

Page 22: VLSI_Design_-_Unit II - Part I

Problem

An inverter fabricated in a 1.2 m CMOS technology uses the minimum possible channel length (i.e., ). If Wn = 1.8 m, find the value of Wp that would result in QN and QP being matched. For this technology,

. Also, calculate the value of the output resistance of the inverter when

S. B. Sivasubramaniyan MSEC, Chennai

1.2n pL L m

2 280 / , 27 / , 0.8 & 5n p tn DDk A V k A V V V V V

o OLv V

Page 23: VLSI_Design_-_Unit II - Part I

Solution We know,

Substituting, we get

S. B. Sivasubramaniyan MSEC, Chennai

pn

p n

W

W

1.8 p

p nW

1.8 p

p n

k

W k

1.8 27

80pW

5.4pW m

Page 24: VLSI_Design_-_Unit II - Part I

Solution

When , NMOS transistor actually provides the path of low resistance given by,

S. B. Sivasubramaniyan MSEC, Chennai

1DSN

n DD tnn

rW

k V VL

o OLv V

2

1

1.880 5 0.8

1.2

DSNr AV

V

0.001984DSN

Vr

A

1.984DSNr k

Page 25: VLSI_Design_-_Unit II - Part I

Assignment

Show that the threshold voltage Vth of a CMOS inverter is given by

Where,

S. B. Sivasubramaniyan MSEC, Chennai

1

DD tp tn

th

r V V VV

r

pp

nn

Wk

Lr

Wk

L

Page 26: VLSI_Design_-_Unit II - Part I

Dynamic Operation

The speed of digital system is characterized by the propagation delay of the individual gates employed in the chip

The inverter propagation delay is the basic parameter with which the propagation delay of the whole system is specified

Here we are going to discuss about the propagation delay of the basic inverter

S. B. Sivasubramaniyan MSEC, Chennai

Page 27: VLSI_Design_-_Unit II - Part I

Dynamic Operation

It is assumed that the input is driven by a pulse with zero rise time and zero fall time

The inverter propagation delay is the basic parameter with which the propagation delay of the whole system is specified

S. B. Sivasubramaniyan MSEC, Chennai

Page 28: VLSI_Design_-_Unit II - Part I

Dynamic Operation

S. B. Sivasubramaniyan MSEC, Chennai

Page 29: VLSI_Design_-_Unit II - Part I

Dynamic Operation - Assumptions

We assume the transistors to be matched This makes tpHL and tpLH to be same Calculating any one of the parameter will help us to

obtain the other We will calculate tpHL For which, we assume that at the instant t = 0+ the

output voltage is at VDD Now transistor QN is ON which would sink large current

S. B. Sivasubramaniyan MSEC, Chennai

Page 30: VLSI_Design_-_Unit II - Part I

Dynamic Operation

The characteristics is shown in the figure

S. B. Sivasubramaniyan MSEC, Chennai

Page 31: VLSI_Design_-_Unit II - Part I

Dynamic Operation

Substituting the expression for current we get,

S. B. Sivasubramaniyan MSEC, Chennai

DN oi dt Cdv

20

1

2n DD t o on

Wk V V v v dt Cdv

L

20

12

nn o

DD t o

Wk

dvLdt

C V V v v

Page 32: VLSI_Design_-_Unit II - Part I

Dynamic Operation

S. B. Sivasubramaniyan MSEC, Chennai

20

1

2

nn o

DD to

DD t

Wk

dvLdt

C V V vv

V V

20

1

2

nn o

DD to

DD t

Wk

dvLdt

C V V vv

V V

Page 33: VLSI_Design_-_Unit II - Part I

Dynamic Operation

S. B. Sivasubramaniyan MSEC, Chennai

Page 34: VLSI_Design_-_Unit II - Part I

Dynamic Operation

Integrating the equation between the limits, VDD – Vt and VDD/2, we get

Also tpHL is denoted as tpHL2

S. B. Sivasubramaniyan MSEC, Chennai

22 2

0

1

2

DD

DD t

Vnn o

pHL V VDD t

oDD t

Wk

dvLt

C V V vv

V V

Page 35: VLSI_Design_-_Unit II - Part I

Dynamic Operation

We know,

S. B. Sivasubramaniyan MSEC, Chennai

2

2

1ln 1

12

DD

DD t

V

pHL

n DD t oDD t V V

Ct

Wk V V vL V V

2

1ln 1

dx

axax x

21

, &2 o

DD t

Here a x vV V

Page 36: VLSI_Design_-_Unit II - Part I

Dynamic Operation

Simplifying,

Total time,

S. B. Sivasubramaniyan MSEC, Chennai

2

3 4ln DD t

pHLDD

n DD t

V VCt

W Vk V VL

1 2pHL pHL pHLt t t

2

3 4ln

12

DD ttpHL

DDn DD t n DD t

V VCV Ct

W W Vk V V k V VL L

Page 37: VLSI_Design_-_Unit II - Part I

Dynamic Operation

Simplifying,

Taking the typical value for threshold voltage

And substituting here, we get

S. B. Sivasubramaniyan MSEC, Chennai

3 42 1

ln2

DD ttpHL

DD t DDn DD t

V VVCt

W V V Vk V VL

0.2t DDV V1.6

pHL

n DDn

Ct

Wk V

L

Page 38: VLSI_Design_-_Unit II - Part I

Dynamic Operation

For tpLH, the same expression applies except for

Which has to replaced by

S. B. Sivasubramaniyan MSEC, Chennai

nn

Wk

L

pp

Wk

L

Page 39: VLSI_Design_-_Unit II - Part I

Propagation Delay

For tp,

S. B. Sivasubramaniyan MSEC, Chennai

2pLH pHL

p

t tt

Page 40: VLSI_Design_-_Unit II - Part I

Propagation Delay - Inference

For tp to be lower, Capacitance should be small Kn’ should be high (W/L) should be high VDD should be high A trade off between above parameters is done to ensure lower propagation

delay

S. B. Sivasubramaniyan MSEC, Chennai

Page 41: VLSI_Design_-_Unit II - Part I

Problem

A CMOS inverter in a VLSI circuit operating from a 10 V supply has

If the total effective load capacitance is 15 pF. Find tp

S. B. Sivasubramaniyan MSEC, Chennai

20, 40,n p

W W

L L

22 20 / , 2 .n ox p ox tn tpC C A V V V V

Page 42: VLSI_Design_-_Unit II - Part I

Solution

We Know

S. B. Sivasubramaniyan MSEC, Chennai

1.6p

n DDn

Ct

Wk V

L

1.6 15

20 20 10p

pFt 6pt ns

Page 43: VLSI_Design_-_Unit II - Part I

Solution

Alternate

S. B. Sivasubramaniyan MSEC, Chennai

3 42 1ln2

t DD tp

DD t DDn DD t

n

V V VCt

W V V Vk V VL

122 15 10 3 10 4 22 1ln

20 20 8 10 2 2 10pt

6pt ns

Page 44: VLSI_Design_-_Unit II - Part I

Assignment

Solution

S. B. Sivasubramaniyan MSEC, Chennai

0.8 , 0.8 , 0.8pLH pHL pt ns t ns t ns

Page 45: VLSI_Design_-_Unit II - Part I

Dynamic Power Dissipation – contd.

The expression for propagation delay can also be derived by taking the average of the currents at VDD (operating point E) and at VDD/2 (operating point F)

S. B. Sivasubramaniyan MSEC, Chennai

Page 46: VLSI_Design_-_Unit II - Part I

Dynamic Power Dissipation – contd.

Device current at E is the saturation current of NMOS transistor, given by

Device current at F is the triode region current of NMOS transistor, given by

S. B. Sivasubramaniyan MSEC, Chennai

20

1

2 n DD tDNn

Wi k V V

L

2

1

2 2 2pHL

DD DDn DD tDN t

n

V VWi k V V

L

Page 47: VLSI_Design_-_Unit II - Part I

Dynamic Power Dissipation – contd.

Average current

The propagation delay is given by (high to low)

S. B. Sivasubramaniyan MSEC, Chennai

0

1

2 pHLDN av DN DN ti i i

pHL

DN av

C Vt

i

/ 2DDpHL

DN av

C Vt

i

Page 48: VLSI_Design_-_Unit II - Part I

Dynamic Power Dissipation – contd.

Propagation delay

Simplifying, we get

S. B. Sivasubramaniyan MSEC, Chennai

2

2

/ 2

1 1 12 2 2 2 2

DDpHL

DD DDn DD t n DD t

n n

C Vt

V VW Wk V V k V V

L L

2 2

12 2 2 2

DDpHL

DD t DD DDn DD t

n

CVt

V V V VWk V V

L

Page 49: VLSI_Design_-_Unit II - Part I

Dynamic Power Dissipation – contd.

Propagation delay

S. B. Sivasubramaniyan MSEC, Chennai

2 20.8

0.82 2 8

DDpHL

DD DD DDn DD

n

CVt

V V VWk V

L

1.7pHL

n DDn

Ct

Wk V

L

Page 50: VLSI_Design_-_Unit II - Part I

Problem

Consider a CMOS inverter fabricated in a 0.25 mm process defined as follows,

Find,

S. B. Sivasubramaniyan MSEC, Chennai

2 2115 / , 30 / , 0.4 ,

0.375 1.1252.5 , , , 6.25

0.25 0.25

n ox p ox tn tp

DD Ln p

C A V C A V V V V

W m W mV V C fF

L m L m

, &pHL pHL pt t t

Page 51: VLSI_Design_-_Unit II - Part I

Solution

The Propagation delay, (high to low)

Where,

S. B. Sivasubramaniyan MSEC, Chennai

/ 2DDpHL

DN av

C Vt

i

0

1

2 pHLDN av DN DN ti i i

Page 52: VLSI_Design_-_Unit II - Part I

Solution

S. B. Sivasubramaniyan MSEC, Chennai

20

1

2 n DD tDNn

Wi k V V

L

20

1 0.375115 2.5 0.42 0.25DN

n

i

0 380DNi A

2

0.375 2.5 1 0.5115 2.5 0.4

0.25 2 2 2pHLDN ti

2

1

2 2 2pHL

DD DDn DD tDN t

n

V VWi k V V

L

318pHLDN t

i A

Page 53: VLSI_Design_-_Unit II - Part I

Solution

Propagation delay,

S. B. Sivasubramaniyan MSEC, Chennai

349DN avi A

1318 380

2DN avi

/ 2DDpHL

DN av

C Vt

i

15

6

6.25 10 1.25

349 10pHLt

23.3pHLt ps

Page 54: VLSI_Design_-_Unit II - Part I

Solution

From the given data,

We see that, the transistors are not matched, The low to high transition will increase by a factor

(3.83/3)

S. B. Sivasubramaniyan MSEC, Chennai

3.83

3pLH pHLt t

3p

n

W

W

& 3.83n

p

1.3 23.3pLHt 30pLHt ps

Page 55: VLSI_Design_-_Unit II - Part I

Solution

Therefore, the actual propagation delay is given by,

S. B. Sivasubramaniyan MSEC, Chennai

1

2p pLH pHLt t t 123.3 30

2pt

26.5pt ps

Page 56: VLSI_Design_-_Unit II - Part I

Assignment

Suppose that an additional load capacitance of 0.1pF is added for the inverter mentioned in the previous problem. Also, in an attempt to decrease the area of the inverter in the previous problem, (W/L)p is made equal to (W/L)n. What is the percentage reduction in area achieved? Find the new values of tpHL, tpLH, and tp.

S. B. Sivasubramaniyan MSEC, Chennai

Page 57: VLSI_Design_-_Unit II - Part I

Current Flow and Power Dissipation

Consider the two characteristics which were already introduced

S. B. Sivasubramaniyan MSEC, Chennai

Page 58: VLSI_Design_-_Unit II - Part I

Current Flow and Power Dissipation

The total energy dissipation in the CMOS inverter in the two cases is given by

If the inverter is switched at the rated of f cycles per second, the dynamic power dissipation is given by

S. B. Sivasubramaniyan MSEC, Chennai

2DDCV

2D DDP fCV

Page 59: VLSI_Design_-_Unit II - Part I

Current Flow and Power Dissipation

We know, frequency of operation is inversely proportional to the propagation delay

The lower the propagation delay (desired) the higher is the power dissipation (not desirable)

A figure of merit referred to as Power Delay product is thus introduced

Power Delay product is given by

S. B. Sivasubramaniyan MSEC, Chennai

D pDP P t

Page 60: VLSI_Design_-_Unit II - Part I

Power Delay product

Power Delay product is a constant, the lower the value of Power Delay product, higher is the effectiveness of the technology

The Power Delay product has the unit of joules It is a measure of energy dissipated per cycle of operation For CMOS technology, the power delay product is simply

S. B. Sivasubramaniyan MSEC, Chennai

2DDDP CV

Page 61: VLSI_Design_-_Unit II - Part I

Problem

Consider a CMOS inverter with , (W/L)n = 20, (W/L)p = 40, , and VDD = 10 V. Find peak current drawn from the supply.

S. B. Sivasubramaniyan MSEC, Chennai

2tn tpV V V 22 20 /n ox p oxC C A V

Page 62: VLSI_Design_-_Unit II - Part I

Solution

For peak current drawn from the supply, Vth = VDD/2 QP and QN both work in the saturation region The current equation if given by

Substituting, we get

S. B. Sivasubramaniyan MSEC, Chennai

21

2DP p DD I tpp

Wi k V V V

L

2

22

1 1010 40 10 2

2 2DP

Ai V

V

Page 63: VLSI_Design_-_Unit II - Part I

Solution

Simplifying, we get

S. B. Sivasubramaniyan MSEC, Chennai

1800 1.8DPi A mA

Page 64: VLSI_Design_-_Unit II - Part I

Problem

Consider a CMOS VLSI chip having 100,000 gates fabricated in a 1.2 m CMOS technology. Let load capacitance per gate be 30 fF. If the chip is operated from a 5V supply and is switched at a rate of 100 MHz, find

The power dissipation per gate The total power dissipated in the chip assuming that only

30 % of the gates are switched at any one time

S. B. Sivasubramaniyan MSEC, Chennai

Page 65: VLSI_Design_-_Unit II - Part I

Solution

Power dissipation per gate is the dynamic power dissipation given by

Substituting,

S. B. Sivasubramaniyan MSEC, Chennai

2DDP fCV

26 15100 10 30 10 5P

75P W

Page 66: VLSI_Design_-_Unit II - Part I

Solution

Total Power dissipation when 30 % of the gates are switched at any one time

S. B. Sivasubramaniyan MSEC, Chennai

3075 100,000

100P W

2.25P W

Page 67: VLSI_Design_-_Unit II - Part I

Problem

Consider a CMOS inverter with , (W/L)n = 20, (W/L)p = 40, , and VDD = 10 V. If the inverter is loaded by 15 pF capacitor, find the dynamic power dissipation when it is switched at a frequency of 2 MHz. What is the average current drawn from the supply?

S. B. Sivasubramaniyan MSEC, Chennai

2tn tpV V V 22 20 /n ox p oxC C A V

Page 68: VLSI_Design_-_Unit II - Part I

Solution 3 mW, 0.3 mA

S. B. Sivasubramaniyan MSEC, Chennai

Assignment

Page 69: VLSI_Design_-_Unit II - Part I

Combinational circuits do not have memory elements

Combinational circuits forms part of every digital systems

S. B. Sivasubramaniyan MSEC, Chennai

Combinational logic design – with CMOS

Page 70: VLSI_Design_-_Unit II - Part I

CMOS logic circuit is just an extension of CMOS inverter

As we know, in a CMOS inverter, a pull-down transistor is formed by a NMOS device and a pull-up transistor is formed by a PMOS device

Similarly, a CMOS logic circuit will have a pull-down network formed by NMOS transistors, and a pull-up network formed by PMOS transistors

S. B. Sivasubramaniyan MSEC, Chennai

Combinational logic design – with CMOS

Page 71: VLSI_Design_-_Unit II - Part I

Pull-down network (PDN) will contain all input combinations that make the output low

Similarly, Pull-up network (PUN) will contain all input combinations that make the output high

We know, Pull-down network is formed by NMOS transistors and NMOS transistors are activated when the gate is high, a PDN network is activated when the gate(input) is high

Similarly, a Pull-up network is activated when the gate(input ) is low

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down and Pull-up network

Page 72: VLSI_Design_-_Unit II - Part I

The inputs to PDN and PUN networks work in a complementary fashion similar to CMOS inverter in which inputs to NMOS and PMOS devices work in a complementary fashion

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down and Pull-up network

Page 73: VLSI_Design_-_Unit II - Part I

The pull-down (and Pull-up) network employs devices in parallel to realize OR function

The pull-down (and Pull-up) network employs devices in series to realize AND function

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down - Basics

Page 74: VLSI_Design_-_Unit II - Part I

Y will be low when A is high or B is high

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down - examples

Page 75: VLSI_Design_-_Unit II - Part I

Y will be low when A is high and B is high

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down - examples

Page 76: VLSI_Design_-_Unit II - Part I

Y will be low when A is high or when B and C are high

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down - examples

Page 77: VLSI_Design_-_Unit II - Part I

The pull-up (and Pull-down) network employs devices in parallel to realize OR function

The pull-up (and Pull-down) network employs devices in series to realize AND function

S. B. Sivasubramaniyan MSEC, Chennai

Pull-up - Basics

Page 78: VLSI_Design_-_Unit II - Part I

The pull-up (and Pull-down) network employs devices in parallel to realize OR function

The pull-up (and Pull-down) network employs devices in series to realize AND function

S. B. Sivasubramaniyan MSEC, Chennai

Pull-up - examples

Page 79: VLSI_Design_-_Unit II - Part I

Y will be high when A is low or B is low

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down - examples

Page 80: VLSI_Design_-_Unit II - Part I

Y will be high only when A and B are low

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down - examples

Page 81: VLSI_Design_-_Unit II - Part I

Y will be high only when A is low or if B and C are both low

S. B. Sivasubramaniyan MSEC, Chennai

Pull-down - examples

Page 82: VLSI_Design_-_Unit II - Part I

Two input NOR gate Two input NAND gate Y = [A(B + CD)]’ Two input Ex-OR gate Three input Ex-OR gate

S. B. Sivasubramaniyan MSEC, Chennai

Assignment