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    ECE 261 Krish Chakrabarty 1

    Performance Characterization

    Delay analysis Transistor sizing Logical effort Power analysis

    ECE 261 Krish Chakrabarty 2

    Delay Definitions

    tpdr: rising propagation delay From input to rising output crossing VDD/2

    tpdf:falling propagation delay From input to falling output crossing VDD/2

    tpd: average propagation delay tpd = (tpdr + tpdf)/2

    tr: rise time

    From output crossing 0.2 VDD to 0.8 VDD

    tf:fall time

    From output crossing 0.8 VDD to 0.2 VDD

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    ECE 261 Krish Chakrabarty 3

    Simulated Inverter Delay Solving differential equations by hand is too hard SPICE simulator solves the equations numerically

    Uses more accurate I-V models too! But simulations take time to write

    ECE 261 Krish Chakrabarty 4

    Delay Estimation We would like to be able to easily estimate delay

    Not as accurate as simulation But easier to ask What if?

    The step response usually looks like a 1st order RCresponse with a decaying exponential.

    Use RC delay models to estimate delay C = total capacitance on output node Use effective resistance R So that t

    pd

    = RC Characterize transistors by finding their effective R

    Depends on average current as gate switches

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    ECE 261 Krish Chakrabarty 5

    RC Delay Models Use equivalent circuits for MOS transistors

    Ideal switch + capacitance and ON resistance Unit nMOS has resistance R, capacitance C Unit pMOS has resistance 2R, capacitance C

    Capacitance proportional to width Resistance inversely proportional to width

    ECE 261 Krish Chakrabarty 6

    Example: 3-input NAND

    Sketch a 3-input NAND with transistor widthschosen to achieve effective rise and fall

    resistances equal to a unit inverter (R).

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    ECE 261 Krish Chakrabarty 7

    Example: 3-input NAND Sketch a 3-input NAND with transistor widths

    chosen to achieve effective rise and fall

    resistances equal to a unit inverter (R).

    ECE 261 Krish Chakrabarty 8

    Example: 3-input NAND Sketch a 3-input NAND with transistor widths

    chosen to achieve effective rise and fall

    resistances equal to a unit inverter (R).

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    ECE 261 Krish Chakrabarty 9

    3-input NAND Caps Annotate the 3-input NAND gate with gate and

    diffusion capacitance.

    ECE 261 Krish Chakrabarty 10

    3-input NAND Caps Annotate the 3-input NAND gate with gate and

    diffusion capacitance.

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    ECE 261 Krish Chakrabarty 11

    3-input NAND Caps Annotate the 3-input NAND gate with gate and

    diffusion capacitance.

    ECE 261 Krish Chakrabarty 12

    Elmore Delay ON transistors look like resistors Pullup or pulldown network modeled asRC ladder Elmore delay of RC ladder

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    ECE 261 Krish Chakrabarty 13

    Example: 2-input NAND Estimate worst-case rising and falling delay of 2-

    input NAND driving h identical gates.

    ECE 261 Krish Chakrabarty 14

    Example: 2-input NAND

    Estimate rising and falling propagation delays of a2-input NAND driving h identical gates.

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    ECE 261 Krish Chakrabarty 15

    Example: 2-input NAND Estimate rising and falling propagation delays of a

    2-input NAND driving h identical gates.

    ECE 261 Krish Chakrabarty 16

    Example: 2-input NAND

    Estimate rising and falling propagation delays of a2-input NAND driving h identical gates.

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    ECE 261 Krish Chakrabarty 17

    Example: 2-input NAND Estimate rising and falling propagation delays of a

    2-input NAND driving h identical gates.

    ECE 261 Krish Chakrabarty 18

    Example: 2-input NAND Estimate rising and falling propagation delays of a

    2-input NAND driving h identical gates.

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    ECE 261 Krish Chakrabarty 19

    Example: 2-input NAND Estimate rising and falling propagation delays of a

    2-input NAND driving h identical gates.

    ECE 261 Krish Chakrabarty 20

    Delay Components

    Delay has two parts Parasitic delay

    6 or 7 RC Independent of load

    Effort delay 4h RC Proportional to load capacitance

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    ECE 261 Krish Chakrabarty 21

    Contamination Delay Best-case (contamination) delay can be

    substantially less than propagation delay. Ex: If both inputs fall simultaneously

    ECE 261 Krish Chakrabarty 22

    Diffusion Capacitance We assumed contacted diffusion on every s / d. Good layout minimizes diffusion area Ex: NAND3 layout shares one diffusion contact

    Reduces output capacitance by 2C Merged uncontacted diffusion might help too

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    ECE 261 Krish Chakrabarty 23

    Layout Comparison Which layout is better?

    ECE 261 Krish Chakrabarty 24

    Resizing the Inverter

    n-diffusion

    Minimum-sized transistor:W=3, L=2

    2

    3

    poly

    2p-diffusion

    poly

    9

    To get equal rise and fall times,n = pWp = 3Wn, assumingthat electron mobility is three times that of holesWp=9

    Sometimes the function

    being implemented

    makes resizing

    unnecessary!

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    ECE 261 Krish Chakrabarty 25

    Analyzing the NAND GateVDD

    ab

    ab

    F

    Gndc

    cn1

    n2n3

    p1 p2 p3 n, eff= 1+

    1n1

    1n2

    1n3

    +

    Resistances are in series (conductancesare in parallel)n1= n2 = n3If then n, eff= n/3

    Pull-down circuit has three times resistance,one-third times the conductance

    = n

    For pull-up, only one transistor has to be on, p, eff= min{p1,p2,p3}p1= p2 = p3If then n, eff= p = p = n/3 no resizing is necessary

    ECE 261 Krish Chakrabarty 26

    Analyzing the NOR Gate

    p, eff= 1+

    1p1

    1p2

    1p3

    +

    Resistances are in series (conductancesare in parallel)p1= p2 = p3If then p, eff= p/3

    Pull-up circuit has three times resistance,one-third times the conductance

    = p

    For pull-down, only one transistor has to be on, n, eff= min{n1,n2,n3}n1= n2 = n3If then n,eff=9p,eff = n = 3p considerable resizing is

    necessaryWp = 9Wn!

    VDDab

    ab

    Gnd

    c

    c

    p1

    p2p3

    n1 n2 n3

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    ECE 261 Krish Chakrabarty 27

    Effect of Series Transistors

    L

    W

    L

    L

    poly

    poly

    poly

    Diffusion

    3L

    W

    Diffusionpoly

    ECE 261 Krish Chakrabarty 28

    Effect of Series Transistors

    VDDab c

    pp

    pPull-down

    Resize the pull-up transistors tomake pull-up times equalAfter resizing: a: 2p, b: 2p, c: p

    Transistorresizingexample

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    ECE 261 Krish Chakrabarty 29

    Transistor Placement (Series Stack)

    Body effect: VtVsb

    a

    b

    F

    Gnd

    c

    Pull-up

    stack

    Ca

    Cb

    Cc

    ta

    tb

    tc

    At time t = 0, a=b=c=0, f=1, capacitances are charged

    Ideally Vta = Vtb = Vtc 0.8V However, Vta > Vtb > Vtc because of

    body effect

    If a, b, c become 1 at the same time, whichtransistor will switch on first?

    How to order transistors in a series stack?

    tc will switch on first (Vsb for tc is zero), Cc willdischarge, pulling Vsb for tb to zero

    If signals arrive at different times, how should the transistors be ordered?

    Design strategy: place latest arriving signal nearestto output-early signals will discharge internal

    nodes

    ECE 261 Krish Chakrabarty 30

    Transistor Placement

    a

    b

    F

    Gnd

    c

    Pull-up

    stack

    Ca

    Cb

    Cc

    ta

    tb

    tcPrimary

    inputs

    (change

    simultaneously)

    2

    2

    2

    2

    a

    bF

    c

    Ca

    Cb

    Cc

    ta

    tb

    tc

    2

    2

    2 2

    Pull-up

    stack

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    ECE 261 Krish Chakrabarty 31

    Some Design Guidelines

    Use NAND gates (instead of NOR) whereverpossible

    Placed inverters (buffers) at high fanout nodes toimprove drive capability

    Avoid use of NOR completely in high-speedcircuits: A1 + A2 + + An = A1.A2.An

    ECE 261 Krish Chakrabarty 32

    Some Design Guidelines Use limited fan-in (

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    ECE 261 Krish Chakrabarty 33

    Logical Effort

    Chip designers face a bewildering array of choices What is the best circuit topology for a function? How many stages of logic give least delay? How wide should the transistors be?

    Logical effort is a method to make these decisions Uses a simple model of delay Allows back-of-the-envelope calculations Helps make rapid comparisons between alternatives Emphasizes remarkable symmetries

    ECE 261 Krish Chakrabarty 34

    Delay in a Logic Gate Express delays in process-independent unit

    = 3RC

    12 ps in 180 nm process

    40 ps in 0.6 m process

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    ECE 261 Krish Chakrabarty 35

    Delay in a Logic Gate Express delays in process-independent unit

    Delay has two components

    ECE 261 Krish Chakrabarty 36

    Delay in a Logic Gate

    Express delays in process-independent unit

    Delay has two components

    Effort delayf= gh (a.k.a. stage effort) Again has two components

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    ECE 261 Krish Chakrabarty 37

    Delay in a Logic Gate Express delays in process-independent unit

    Delay has two components Effort delayf = gh (a.k.a. stage effort)

    Again has two components g: logical effort

    Measures relative ability of gate to deliver current g 1 for inverter

    ECE 261 Krish Chakrabarty 38

    Delay in a Logic Gate Express delays in process-independent unit

    Delay has two components Effort delayf = gh (a.k.a. stage effort)

    Again has two components h: electrical effort= C

    out

    / Cin

    Ratio of output to input capacitance Sometimes called fanout

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    ECE 261 Krish Chakrabarty 39

    Delay in a Logic Gate Express delays in process-independent unit

    Delay has two components Parasitic delay p

    Represents delay of gate driving no load

    Set by internal parasitic capacitance

    ECE 261 Krish Chakrabarty 40

    Delay Plots

    d = f+ p = gh + p

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    ECE 261 Krish Chakrabarty 41

    Delay Plots

    d =f+p = gh +p

    ECE 261 Krish Chakrabarty 42

    Computing Logical Effort Definition:Logical effort is the ratio of the input

    capacitance of a gate to the input capacitance of

    an inverter delivering the same output current. Measure from delay vs. fanout plots Or estimate by counting transistor widths

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    ECE 261 Krish Chakrabarty 43

    Catalog of Gates

    Gate type Number of inputs1 2 3 4 n

    Inverter 1NAND 4/3 5/3 6/3 (n+2)/3NOR 5/3 7/3 9/3 (2n+1)/3Tristate / mux 2 2 2 2 2

    Logical effort of common gates

    ECE 261 Krish Chakrabarty 44

    Catalog of Gates

    Gate type Number of inputs1 2 3 4 n

    Inverter 1NAND 2 3 4 nNOR 2 3 4 nTristate / mux 2 4 6 8 2nXOR, XNOR 4 6 8

    Parasitic delay of common gates In multiples of pinv (1)

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    ECE 261 Krish Chakrabarty 45

    Example: Ring Oscillator Estimate the frequency of an N-stage ring oscillator

    Logical Effort: g = Electrical Effort: h =Parasitic Delay: p =Stage Delay: d =Frequency: fosc =

    ECE 261 Krish Chakrabarty 46

    Example: Ring Oscillator

    Estimate the frequency of an N-stage ring oscillator

    Logical Effort: g = 1Electrical Effort: h = 1Parasitic Delay: p = 1Stage Delay: d = 2Frequency: fosc = 1/(2*N*d) = 1/4N

    31 stage ring oscillator in

    0.6 m process hasfrequency of ~ 200 MHz

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    ECE 261 Krish Chakrabarty 47

    Example: FO4 Inverter Estimate the delay of a fanout-of-4 (FO4) inverter

    Logical Effort: g = Electrical Effort: h =Parasitic Delay:

    p =

    Stage Delay: d =

    ECE 261 Krish Chakrabarty 48

    Example: FO4 Inverter Estimate the delay of a fanout-of-4 (FO4) inverter

    Logical Effort: g = 1Electrical Effort: h = 4Parasitic Delay: p = 1Stage Delay: d = 5

    The FO4 delay is about

    200 ps in 0.6 m process

    60 ps in a 180 nm process

    f/3 ns in an fm process

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    ECE 261 Krish Chakrabarty 49

    Multistage Logic Networks Logical effort generalizes to multistage networks Path Logical Effort Path Electrical Effort Path Effort

    ECE 261 Krish Chakrabarty 50

    Multistage Logic Networks Logical effort generalizes to multistage networks Path Logical Effort Path Electrical Effort Path Effort Can we write F = GH?

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    ECE 261 Krish Chakrabarty 51

    Paths that Branch

    No! Consider paths that branch:G =H =GH=h

    1

    =h2 =F = GH?

    ECE 261 Krish Chakrabarty 52

    Paths that Branch

    No! Consider paths that branch:G = 1H = 90 / 5 = 18GH= 18h1

    = (15 +15) / 5 = 6

    h2 = 90 / 15 = 6F = g1g2h1h2 = 36 = 2GH

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    ECE 261 Krish Chakrabarty 53

    Branching Effort Introduce branching effort

    Accounts for branching between stages in path

    Now we compute the path effort F = GBH

    Note:

    ECE 261 Krish Chakrabarty 54

    Multistage Delays

    Path Effort Delay Path Parasitic Delay Path Delay

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    ECE 261 Krish Chakrabarty 55

    Designing Fast Circuits

    Delay is smallest when each stage bears same effort

    Thus minimum delay of N stage path is

    This is a key result of logical effort

    Find fastest possible delay Doesnt require calculating gate sizes

    ECE 261 Krish Chakrabarty 56

    Gate Sizes How wide should the gates be for least delay?

    Working backward, apply capacitance transformation tofind input capacitance of each gate given load it drives.

    Check work by verifying input cap spec is met.

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    ECE 261 Krish Chakrabarty 57

    Example: 3-stage path

    Select gate sizes x and y for least delay from A toB

    ECE 261 Krish Chakrabarty 58

    Example: 3-stage path

    Logical Effort G = Electrical Effort H =Branching Effort B =Path Effort F =Best Stage Effort Parasitic Delay P =Delay D =

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    ECE 261 Krish Chakrabarty 59

    Example: 3-stage path

    Logical Effort G = (4/3)*(5/3)*(5/3) = 100/27Electrical Effort H = 45/8Branching Effort B = 3 * 2 = 6Path Effort F = GBH = 125Best Stage Effort Parasitic Delay P = 2 + 3 + 2 = 7Delay D = 3*5 + 7 = 22 = 4.4 FO4

    ECE 261 Krish Chakrabarty 60

    Example: 3-stage path

    Work backward for sizesy =x =

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    ECE 261 Krish Chakrabarty 61

    Example: 3-stage path Work backward for sizes

    y = 45 * (5/3) / 5 = 15x = (15*2) * (5/3) / 5 = 10

    ECE 261 Krish Chakrabarty 62

    Best Number of Stages How many stages should a path use?

    Minimizing number of stages is not always fastest Example: drive 64-bit datapath with unit inverter

    D =

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    ECE 261 Krish Chakrabarty 63

    Best Number of Stages How many stages should a path use?

    Minimizing number of stages is not always fastest Example: drive 64-bit datapath with unit inverter

    D = NF1/N + P = N(64)1/N + N

    ECE 261 Krish Chakrabarty 64

    Derivation Consider adding inverters to end of path

    How many give least delay?

    Defi

    ne best stage effort

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    ECE 261 Krish Chakrabarty 65

    Best Stage Effort

    has no closed-form solution Neglecting parasitics (pinv = 0), we find = 2.718

    (e) For pinv = 1, solve numerically for = 3.59

    ECE 261 Krish Chakrabarty 66

    Review of DefinitionsTerm Stage Pathnumber of stageslogical effortelectrical effortbranching effortefforteffort delayparasitic delaydelay

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    ECE 261 Krish Chakrabarty 67

    Method of Logical Effort1) Compute path effort2) Estimate best number of stages3) Sketch path with N stages4) Estimate least delay5) Determine best stage effort6) Find gate sizes

    ECE 261 Krish Chakrabarty 68

    Limits of Logical Effort

    Chicken and egg problem Need path to compute G But dont know number of stages without G

    Simplistic delay model Neglects input rise time effects

    Interconnect

    Iteration required in designs with wire

    Maximum speed only

    Not minimum area/power for constrained delay

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    ECE 261 Krish Chakrabarty 69

    Summary

    Logical effort is useful for thinking of delay in circuits Numeric logical effort characterizes gates NANDs are faster than NORs in CMOS Paths are fastest when effort delays are ~4 Path delay is weakly sensitive to stages, sizes But using fewer stages doesnt mean faster paths Delay of path is about log4F FO4 inverter delays Inverters and NAND2 best for driving large caps

    Provides language for discussing fast circuits But requires practice to master

    ECE 261 Krish Chakrabarty 70

    Power and Energy

    Power is drawn from a voltage source attached tothe VDD pin(s) of a chip.

    Instantaneous Power: Energy: Average Power:

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    ECE 261 Krish Chakrabarty 71

    Dynamic Power Dynamic power is required to charge and discharge load

    capacitances when transistors switch. One cycle involves a rising and falling output. On rising output, charge Q = CVDD is required On falling output, charge is dumped to GND This repeats Tfsw timesover an interval of T

    ECE 261 Krish Chakrabarty 72

    Dynamic Power Cont.

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    ECE 261 Krish Chakrabarty 73

    Dynamic Power Cont.

    ECE 261 Krish Chakrabarty 74

    Activity Factor

    Suppose the system clock frequency = f Let fsw = f, where = activity factor

    If the signal is a clock, = 1 If the signal switches once per cycle, = Dynamic gates:

    Switch either 0 or 2 times per cycle, = Static gates:

    Depends on design, but typically = 0.1 Dynamic power:

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    ECE 261 Krish Chakrabarty 75

    Short Circuit Current

    When transistors switch, both nMOS and pMOSnetworks may be momentarily ON at once

    Leads to a blip of short circuit current. < 10% of dynamic power if rise/fall times are

    comparable for input and output

    ECE 261 Krish Chakrabarty 76

    Example

    200 Mtransistor chip 20M logic transistors

    Average width: 12 180M memory transistors

    Average width: 4 1.2 V 100 nm process Cg = 2 fF/m

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    ECE 261 Krish Chakrabarty 77

    Dynamic Example

    Static CMOS logic gates: activity factor = 0.1 Memory arrays: activity factor = 0.05 (many

    banks!) Estimate dynamic power consumption per MHz.

    Neglect wire capacitance and short-circuit current.

    ECE 261 Krish Chakrabarty 78

    Dynamic Example Static CMOS logic gates: activity factor = 0.1 Memory arrays: activity factor = 0.05 (many

    banks!) Estimate dynamic power consumption per MHz.

    Neglect wire capacitance.

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    ECE 261 Krish Chakrabarty 79

    Static Power Static power is consumed even when chip is

    quiescent. Ratioed circuits burn power in fight between ON

    transistors Leakage draws power from nominally OFF devices

    ECE 261 Krish Chakrabarty 80

    Ratio Example The chip contains a 32 word x 48 bit ROM

    Uses pseudo-nMOS decoder and bitline pullups On average, one wordline and 24 bitlines are high

    Find static power drawn by the ROM = 75 A/V2 Vtp = -0.4V

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    ECE 261 Krish Chakrabarty 81

    Ratio Example The chip contains a 32 word x 48 bit ROM

    Uses pseudo-nMOS decoder and bitline pullups On average, one wordline and 24 bitlines are high

    Find static power drawn by the ROM = 75 A/V2 Vtp = -0.4V

    Solution:

    ECE 261 Krish Chakrabarty 82

    Leakage Example

    The process has two threshold voltages and two oxidethicknesses.

    Subthreshold leakage: 20 nA/m for low Vt 0.02 nA/m for high Vt

    Gate leakage: 3 nA/m for thin oxide 0.002 nA/m for thick oxide

    Memories use low-leakage transistors everywhere Gates use low-leakage transistors on 80% of logic

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    ECE 261 Krish Chakrabarty 83

    Leakage Example Cont.

    Estimate static power:

    ECE 261 Krish Chakrabarty 84

    Leakage Example Cont. Estimate static power:

    High leakage: Low leakage:

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    ECE 261 Krish Chakrabarty 85

    Leakage Example Cont.

    Estimate static power: High leakage: Low leakage:

    If no low leakage devices, Pstatic = 749 mW (!)

    ECE 261 Krish Chakrabarty 86

    Low Power Design

    Reduce dynamic power : C: VDD: f:

    Reduce static power

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    ECE 261 Krish Chakrabarty 87

    Low Power Design

    Reduce dynamic power : clock gating, sleep mode C: VDD: f:

    Reduce static power

    ECE 261 Krish Chakrabarty 88

    Low Power Design

    Reduce dynamic power : clock gating, sleep mode C: small transistors (esp. on clock), short wires VDD: f:

    Reduce static power

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    ECE 261 Krish Chakrabarty 89

    Low Power Design

    Reduce dynamic power : clock gating, sleep mode C: small transistors (esp. on clock), short wires VDD: lowest suitable voltage f:

    Reduce static power

    ECE 261 Krish Chakrabarty 90

    Low Power Design

    Reduce dynamic power : clock gating, sleep mode C: small transistors (esp. on clock), short wires VDD: lowest suitable voltage f: lowest suitable frequency

    Reduce static power

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    ECE 261 Krish Chakrabarty 91

    Low Power Design

    Reduce dynamic power : clock gating, sleep mode C: small transistors (esp. on clock), short wires VDD: lowest suitable voltage f: lowest suitable frequency

    Reduce static power Selectively use ratioed circuits Selectively use low V

    t

    devices Leakage reduction:

    stacked devices, body bias, low temperature