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Low-Power Design and Test
Logic-Level Power Estimation
Vishwani D. Agrawal
Srivaths Ravi
Auburn University, USA
Texas Instruments India
[email protected]
[email protected]
Hyderabad, July 30-31, 2007
http://www.eng.auburn.edu/~vagrawal/hyd.html
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
1
Power Analysis
 Motivation:
 Specification
 Optimization
 Reliability
 Applications




Design analysis and optimization
Physical design
Packaging
Test
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
2
Abstraction, Complexity, Accuracy
Abstraction level
Algorithm
Computing resources
Analysis accuracy
Least
Worst
Most
Best
Software and system
Hardware behavior
Register transfer
Logic
Circuit
Device
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
3
Spice
 Circuit/device level analysis
 Circuit modeled as network of transistors, capacitors, resistors
and voltage/current sources.
 Node current equations using Kirchhoff’s current law.
 Average and instantaneous power computed from supply
voltage and device current.
 Analysis is accurate but expensive
 Used to characterize parts of a larger circuit.
 Original references:
 L. W. Nagel and D. O. Pederson, “SPICE – Simulation Program
With Integrated Circuit Emphasis,” Memo ERL-M382, EECS
Dept., University of California, Berkeley, Apr. 1973.
 L. W. Nagel, SPICE 2, A Computer program to Simulate
Semiconductor Circuits, PhD Dissertation, University of
California, Berkeley, May 1975.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
4
Logic Model of MOS Circuit
pMOS FETs
VDD
a
a
Ca
c
Cc
b
Cb nMOS
FETs
Cd
Ca , Cb , Cc and Cd are
node capacitances
Copyright Agrawal & Srivaths, 2007
b
Da
Dc
c
Db
Da and Db are
interconnect or
propagation delays
Dc is inertial delay
of gate
Low-Power Design and Test, Lecture 3
5
Spice Characterization of a 2-Input
NAND Gate
Input data pattern
Delay (ps)
Dynamic energy (pJ)
a=b=0→1
69
1.55
a = 1, b = 0 → 1
62
1.67
a = 0 → 1, b = 1
50
1.72
a=b=1→0
35
1.82
a = 1, b = 1 → 0
76
1.39
a = 1 → 0, b = 1
57
1.94
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
6
Spice Characterization (Cont.)
Input data pattern
Static power (pW)
a=b=0
5.05
a = 0, b = 1
13.1
a = 1, b = 0
5.10
a=b=1
28.5
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
7
Switch-Level Partitioning
 Circuit partitioned into channel-connected components
for Spice characterization.
 Reference: R. E. Bryant, “A Switch-Level Model and
Simulator for MOS Digital Systems,” IEEE Trans.
Computers, vol. C-33, no. 2, pp. 160-177, Feb. 1984.
Internal
switching
nodes not
seen by
logic
simulator
Copyright Agrawal & Srivaths, 2007
G2
G1
G3
Low-Power Design and Test, Lecture 3
8
Delay and Discrete-Event Simulation
Inputs
(NAND gate)
Transient
region
a
b
c (CMOS)
Logic simulation
c (zero delay)
c (unit delay)
X
c (multiple delay)
Unknown (X)
c (minmax delay)
0
Copyright Agrawal & Srivaths, 2007
5
Low-Power Design and Test, Lecture 3
rise=5, fall=5
min =2, max =5
Time units
9
Event-Driven Simulation Example
Scheduled
events
a =1
c =1→0
e =1
g =1
2
2
d=0
4
b =1
f =0
Time stack
2
t=0
1
2
3
4
5
6
7
8
Activity
list
c=0
d, e
d = 1, e = 0
f, g
g=0
f=1
g
g=1
g
0
4
Copyright Agrawal & Srivaths, 2007
8
Time, t
Low-Power Design and Test, Lecture 3
10
Time Wheel (Circular Stack)
Current
time
pointer
max
t=0
1
Event link-list
2
3
4
5
6
7
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
11
Gate-Level Power Analysis
 Pre-simulation analysis:
 Partition circuit into channel connected gate
components.
 Determine node capacitances from layout
analysis (accurate) or from wire-load model*
(approximate).
 Determine dynamic and static power from Spice
for each gate.
 Determine gate delays using Spice or Elmore
delay model.
* Wire-load model estimates capacitance of a net by its pin-count.
See Yeap, p. 39.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
12
Elmore Delay Model
 W. Elmore, “The Transient Response of Damped Linear Networks
with Particular Regard to Wideband Amplifiers,” J. Appl. Phys., vol.
19, no.1, pp. 55-63, Jan. 1948.
2
R2
C2
1
R1
s
4
R4
C1
C4
R3
3
Shared resistance:
R5
C3
R45 = R1 + R3
R15 = R1
R34 = R1 + R3
Copyright Agrawal & Srivaths, 2007
5
C5
Low-Power Design and Test, Lecture 3
13
Elmore Delay Formula
N
Delay at node k = 0.69 Σ Cj × Rjk
j=1
where N = number of capacitive nodes in the network
Example:
Delay at node 5 = 0.69[R1 C1 + R1 C2 + (R1+R3)C3 + (R1+R3)C4
+ (R1+R3+R5)C5]
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
14
Gate-Level Power Analysis (Cont.)
 Run discrete-event (event-driven) logic
simulation with a set of input vectors.
 Monitor the toggle count of each net and obtain
capacitive power dissipation:
Pcap = Σ Ck V 2 f
all nodes k
 Where:
 Ck is the total node capacitance being switched, as
determined by the simulator.
 V is the supply voltage.
 f is the clock frequency, i.e., the number of vectors applied
per unit time
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
15
Gate-Level Power Analysis (Cont.)
 Monitor dynamic energy events at the
input of each gate and obtain internal
switching power dissipation:
Pint = Σ
Σ E(g,e) F(g,e)
gates g
events e
 Where
 E(g,e) = energy of event e of gate g, precomputed from Spice.
 F(g,e) = occurrence frequency of the event e at
gate g, observed by logic simulation.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
16
Gate-Level Power Analysis (Cont.)
 Monitor the static power dissipation state of
each gate and obtain the static power
dissipation:
Pstat = Σ
gates g
Σ P(g,s) T(g,s)/ T
states s
 Where
 P(g,s) = static power dissipation of gate g for state s,
obtained from Spice.
 T(g,s) = duration of state s at gate g, obtained from logic
simulation.
 T = vector period.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
17
Gate-Level Power Analysis
 Sum up all three components of power:
P = Pcap + Pint + Pstat
 References:
 A. Deng, “Power Analysis for CMOS/BiCMOS Circuits,” Proc.
International Workshop Low Power Design, 1994.
 J. Benkoski, A. C. Deng, C. X. Huang, S. Napper and J. Tuan,
“Simulation Algorithms, Power Estimation and Diagnostics in
PowerMill,” Proc. PATMOS, 1995.
 C. X. Huang, B. Zhang, A. C. Deng and B. Swirski, “The
Design and Implementation of PowerMill,” Proc. International
Symp. Low Power Design, 1995, pp. 105-109.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
18
Probabilistic Analysis
 View signals as a random processes
Prob{s(t) = 1} = p1
p0 = 1 – p1
C
0→1 transition probability = (1 – p1) p1
Power, P = (1 – p1) p1 CV2fck
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
19
Source of Inaccuracy
p1 = 0.5
P = 0.5CV 2 fck
1/fck
p1 = 0.5
P = 0.33CV 2 fck
p1 = 0.5
P = 0.167CV 2 fck
Observe that the formula, Power, P = (1 – p1) p1 C V 2 fck , is not
Correct.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
20
Switching Frequency
Number of transitions per unit time:
T
=
N(t)
───
t
For a continuous signal:
T
=
lim
t→∞
N(t)
───
t
T is defined as transition density.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
21
Static Signal Probabilities
 Observe signal for interval t 0 + t 1
 Signal is 1 for duration t 1
 Signal is 0 for duration t 0
 Signal probabilities:
 p 1 = t 1/(t 0 + t 1)
 p 0 = t 0/(t 0 + t 1) = 1 – p 1
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
22
Static Transition Probabilities
 Transition probabilities:
 T 01 = p 0 Prob{signal is 1 | signal was 0} = p 0 p1
 T 10 = p 1 Prob{signal is 0 | signal was 1} = p 1 p 0
 T = T 01 + T 10 = 2 p 0 p 1 = 2 p 1 (1 – p 1)
 Transition density: T = 2 p 1 (1 – p 1)
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
23
Static Transition Frequency
f = p1(1 – p1)
0.25
0.2
0.1
0.0
0
Copyright Agrawal & Srivaths, 2007
0.25
0.5
p1
0.75
Low-Power Design and Test, Lecture 3
1.0
24
Inaccuracy in Transition Density
p1 = 0.5
T = 1.0
1/fck
p1 = 0.5
T = 4/6
p1 = 0.5
T = 1/6
Observe that the formula, T = 2 p1 (1 – p1), is not correct.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
25
Cause for Error and Correction
 Probability of transition is not independent of
the present state of the signal.
 Determine probability p 01 of a 0→1
transition.
 Recognize p 01 ≠ p 0 × p 1
 We obtain p 1 = (1 – p 1)p 01 + p 1 p 11
p 01
p 1 = ─────────
1 – p 11 + p 01
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
26
Correction (Cont.)
 Since p 11 + p 10 = 1, i.e., given that the
signal was previously 1, its present value
can be either 1 or 0.
 Therefore,
p 01
p 1 = ──────
p 10 + p 01
This uniquely gives signal probability as a
function of transition probabilities.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
27
Transition and Signal Probabilities
p01 = p10 = 0.5
p1 = 0.5
1/fck
p01 = p10 = 1/3
p1 = 0.5
p01 = p10 = 1/6
p1 = 0.5
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
28
Probabilities: p0, p1, p00, p01, p10, p11
 p 01 + p 00 =1
 p 11 + p 10 = 1
 p0=1–p1
p 01
p 1 = ───────
p 10 + p 01
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
29
Transition Density
 T = 2 p 1 (1 – p 1) = p 0 p 01 + p 1 p 10
= 2 p 10 p 01 / (p 10 + p 01)
= 2 p 1 p 10 = 2 p 0 p 01
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
30
Power Calculation
 Power can be estimated if transition density
is known for all signals.
 Calculation of transition density requires
 Signal probabilities
 Transition densities for primary inputs;
computed from vector statistics
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
31
Signal Probabilities
x1
x1 x2
x2
x1
x1 + x2 – x1x2
x2
1 - x1
x1
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
32
Signal Probabilities
x1
x2
x3
X1
0
0
0
0
1
1
1
1
X2
0
0
1
1
0
0
1
1
0.5
x1 x2
0.25
0.5
0.625
0.5
X3
0
1
0
1
0
1
0
1
Copyright Agrawal & Srivaths, 2007
Y
1
0
1
0
1
0
1
1
y = 1 - (1 - x1x2) x3
= 1 - x3 + x1x2x3
= 0.625
Ref: K. P. Parker and E. J. McCluskey,
“Probabilistic Treatment of General
Combinational Networks,” IEEE Trans.
on Computers, vol. C-24, no. 6, pp. 668670, June 1975.
Low-Power Design and Test, Lecture 3
33
Correlated Signal Probabilities
x1
0.5
x1 x2
0.5
0.25
0.625?
x2
X1
0
0
1
1
X2
0
1
0
1
Copyright Agrawal & Srivaths, 2007
y = 1 - (1 - x1x2) x2
= 1 – x2 + x1x2x2
= 1 – x2 + x1x2
= 0.75 (correct value)
Y
1
0
1
1
Low-Power Design and Test, Lecture 3
34
Correlated Signal Probabilities
x1
x2
X1
0
0
1
1
0.5
x1 + x2 – x1x2
0.5
0.75
X2
0
1
0
1
Copyright Agrawal & Srivaths, 2007
0.375?
y = (x1 + x2 – x1x2) x2
= x1x2 + x2x2 – x1x2x2
= x1x2 + x2 – x1x2
= x2
= 0.5 (correct value)
Y
0
1
0
1
Low-Power Design and Test, Lecture 3
35
Observation
 Numerical computation of signal
probabilities is accurate for fanout-free
circuits.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
36
Remedies
 Use Shannon’s expansion theorem to
compute signal probabilities.
 Use Boolean difference formula to compute
transition densities.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
37
Shannon’s Expansion Theorem
 C. E. Shannon, “A Symbolic Analysis of Relay
and Switching Circuits,” Trans. AIEE, vol. 57, pp.
713-723, 1938.
 Consider:
 Boolean variables, X1, X2, . . . , Xn
 Boolean function, F(X1, X2, . . . , Xn)
 Then F = Xi F(Xi=1) + Xi’ F(Xi=0)
 Where
 Xi’ is complement of X1
 Cofactors, F(Xi=j) = F(X1, X2, . . , Xi=j, . . , Xn), j = 0 or 1
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
38
Expansion About Two Inputs
 F = XiXj F(Xi=1, Xj=1) + XiXj’ F(Xi=1, Xj=0)
+ Xi’Xj F(Xi=0, Xj=1)
+ Xi’Xj’ F(Xi=0, Xj=0)
 In general, a Boolean function can be
expanded about any number of input
variables.
 Expansion about k variables will have 2k
terms.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
39
Correlated Signal Probabilities
X1
X1 X2
Y = X1 X2 + X2’
X2
X1
0
0
1
1
X2
0
1
0
1
Copyright Agrawal & Srivaths, 2007
Y
1
0
1
1
Shannon expansion about the
reconverging input, X2:
Y = X2 Y(X2 = 1) + X2’ Y(X2 = 0)
= X2 (X1) + X2’ (1)
Low-Power Design and Test, Lecture 3
40
Correlated Signals
 When the output function is expanded about all
reconverging input variables,
 All cofactors correspond to fanout-free circuits.
 Signal probabilities for cofactor outputs can be calculated
without error.
 A weighted sum of cofactor probabilities gives the correct
probability of the output.
 For two reconverging inputs:
f = xixj f(Xi=1, Xj=1) + xi(1-xj) f(Xi=1, Xj=0)
+ (1-xi)xj f(Xi=0, Xj=1) + (1-xi)(1-xj) f(Xi=0, Xj=0)
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
41
Correlated Signal Probabilities
X1
X1 X2
Y = X1 X2 + X2’
X2
X1
0
0
1
1
X2
0
1
0
1
Y
1
0
1
1
Shannon expansion about the
reconverging input, X2:
Y = X2 Y(X2=1) + X2’ Y(X2=0)
= X2 (X1) + X2’ (1)
y = x2 (0.5) + (1-x2) (1)
= 0.5 (0.5) + (1-0.5) (1)
= 0.75
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
42
Example
0.5
Supergate
0.25
0.5
0.0
0.5
1
0
0.0 0.5
1.0
0.5
Reconv.
signal
Point of
reconv.
0.5
1.0
0.375
Signal probability for supergate output
= 0.5 Prob{rec. signal = 1} + 1.0 Prob{rec. signal = 0}
= 0.5 × 0.5 + 1.0 × 0.5 = 0.75
S. C. Seth and V. D. Agrawal, “A New Model for Computation of
Probabilistic Testability in Combinational Circuits,” Integration, the VLSI
Journal, vol. 7, no. 1, pp. 49-75, April 1989.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
43
Probability Calculation Algorithm
 Partition circuit into supergates.
 Definition: A supergate is a circuit partition with a single output
such that all fanouts that reconverge at the output are contained
within the supergate.
 Identify reconverging and non-reconverging inputs
of each supergate.
 Compute signal probabilities from PI to PO:
 For a supergate whose input probabilities are known
 Enumerate reconverging input states
 For each input state do gate by gate probability computation
 Sum up corresponding signal probabilities, weighted by state
probabilities
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
44
Calculating Transition Density
..
..
.
1
x1, T1
xn, Tn
Copyright Agrawal & Srivaths, 2007
Boolean
function
y, T(Y) = ?
n
Low-Power Design and Test, Lecture 3
45
Boolean Difference
Boolean diff(Y, Xi) =
∂Y
── = Y(Xi=1) ⊕ Y(Xi=0)
∂Xi
 Boolean diff(Y, Xi) = 1 means that a path is sensitized from input Xi
to output Y.
 Prob(Boolean diff(Y, Xi) = 1) is the probability of transmitting a
toggle from Xi to Y.
 Probability of Boolean difference is determined from the probabilities
of cofactors of Y with respect to Xi.
F. F. Sellers, M. Y. Hsiao and L. W. Bearnson, “Analyzing Errors with
the Boolean Difference,” IEEE Trans. on Computers, vol. C-17, no. 7,
pp. 676-683, July 1968.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
46
Transition Density
n
T(y) = Σ T(Xi) Prob(Boolean diff(Y, Xi) = 1)
i=1
F. Najm, “Transition Density: A New Measure of Activity in Digital
Circuits,” IEEE Trans. CAD, vol. 12, pp. 310-323, Feb. 1993.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
47
Power Computation
 For each primary input, determine signal probability and
transition density for given vectors.
 For each internal node and primary output Y, find the
transition density T(Y), using supergate partitioning and
the Boolean difference formula.
 Compute power,
P=
Σ
0.5CY V2 T(Y)
all Y
where CY is the capacitance of node Y and V is supply
voltage.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
48
Transition Density and Power
X1
X2
X3
0.2, 1
0.3, 2
0.06, 0.7
0.436, 3.24
Ci
Y
0.4, 3
CY
Transition density
Signal probability
Power = 0.5 V 2 (0.7Ci + 3.24CY)
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
49
Prob. Method vs. Logic Sim.
Probability method
Logic Simulation
Circuit
No. of
gates
Av. density
CPU s*
Av. density
CPU s*
Error
%
C432
160
3.46
0.52
3.39
63
+2.1
C499
202
11.36
0.58
8.57
241
+29.8
C880
383
2.78
1.06
3.25
132
-14.5
C1355
346
4.19
1.39
6.18
408
-32.2
C1908
880
2.97
2.00
5.01
464
-40.7
C2670
1193
3.50
3.45
4.00
619
-12.5
C3540
1669
4.47
3.77
4.49
1082
-0.4
C5315
2307
3.52
6.41
4.79
1616
-26.5
C6288
2406
25.10
5.67
34.17
31057
-26.5
3.83
9.85
5.08
2713
-24.2
C7552 3512
* CONVEX c240
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
50
Probability Waveform Methods
 F. Najm, R. Burch, P. Yang and I. Hajj, “CREST – A
Current Estimator for CMOS Circuits,” Proc. IEEE Int.
Conf. on CAD, Nov. 1988, pp. 204-207.
 C.-S. Ding, et al., “Gate-Level Power Estimation using
Tagged Probabilistic Simulation,” IEEE Trans. on CAD, vol.
17, no. 11, pp. 1099-1107, Nov. 1998.
 F. Hu and V. D. Agrawal, “Dual-Transition Glitch Filtering
in Probabilistic Waveform Power Estimation,” Proc. IEEE
Great Lakes Symp. VLSI, Apr. 2005, pp. 357-360.
 F. Hu and V. D. Agrawal, “Enhanced Dual-Transition
Probabilistic Power Estimation with Selective Supergate
Analysis,” Proc. IEEE Int. Conf. Computer Design, Oct.
2005. pp. 366-369.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
51
Problem 1
For equiprobable inputs analyze the 0→1 transition probabilities of all
gates in the two implementations of a four-input AND gate shown
below. Assuming that the gates have zero delays, which
implementation will consume less average dynamic power?
E
A
B
C
D
F
Chain structure
Copyright Agrawal & Srivaths, 2007
G
E
A
B
C
D
G
F
Tree structure
Low-Power Design and Test, Lecture 3
52
Problem 1 Solution
Given the primary input probabilities, P(A) = P(B) = P(C) = P(D) = 0.5,
signal and transition (0→1) probabilities are as follows:
Signal
name
Chain
Tree
Prob(sig.= 1) Prob(0→1) Prob(sig.=1)
Prob(0→1)
E
0.2500
0.1875
0.2500
0.1875
F
0.1250
0.1094
0.2500
0.1875
G
0.0625
0.0586
0.0625
0.0586
Total
transitions/vector
0.3555
0.4336
The tree implementation consumes 100×(0.4336 – 0.3555)/0.3555 = 22%
more average dynamic power. This advantage of the chain structure may
be somewhat reduced because of glitches caused by unbalanced path
delays.
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
53
Problem 2
Assume that the two-input AND gates in Problem 1 each has one unit
of delay. Find input vector pairs for each implementation that will
consume the peak dynamic power. Which implementation consumes
less peak dynamic power?
E
A
B
C
D
F
Chain structure
Copyright Agrawal & Srivaths, 2007
G
E
A
B
C
D
G
F
Tree structure
Low-Power Design and Test, Lecture 3
54
Problem 2 Solution
For the chain structure, a vector pair {A B C D} = {1110},{1011} will
produce four gate transitions as shown below.
A
E
F
B
C
D
G
A=11
B=10
E=10
C=11
F=10
D=01
G=00
0
Copyright Agrawal & Srivaths, 2007
1
2
3
Time units
Low-Power Design and Test, Lecture 3
55
Problem 2 Solution (Cont.)
The tree structure has balanced delay paths. So it cannot make more
than 3 gate transitions. A vector pair {ABCD} = {1111},{1010} will
produce three transitions as shown below.
A
E
B
G
C
D
F
A=11
Therefore, just counting the gate
transitions, we find that the chain
consumes 100(4 – 3)/3 = 33%
higher peak power than the tree.
B=10
E=10
C=11
D=10
F=10
G=10
Time units
0
1
2
3
Copyright Agrawal & Srivaths, 2007
Low-Power Design and Test, Lecture 3
56
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