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U. Glaeser

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Total Average Power<br />

Putting together all the components of power dissipation, the total average power consumption of a logic<br />

gate can be expressed as follows:<br />

Ptotal = Pdynamic + Pdirect-path + Pstatic =<br />

© 2002 by CRC Press LLC<br />

(20.1)<br />

Among these components, dynamic power is by far the most dominant component and accounts for<br />

more than 80% of the total power consumption in modern day CMOS technology. Thus, the total average<br />

power for all logic gates in the circuits can be approximated by summing up all the dynamic component<br />

of each of the logic gate,<br />

where n is the number of logic gates in the circuit.<br />

Power Due to the Internal Nodes of a Logic Gate<br />

The power consumption due to the internal nodes of the logic gates has been ignored in the above<br />

analysis, which causes inaccuracy in the power consumption result. The internal node capacitances are<br />

primarily due to the source and drain diffusion capacitances of the transistors, and are not as large as<br />

the output node capacitance. Hence, total power consumption is still dominated by the charging and<br />

discharging of the output node capacitances. Nevertheless, depending on the applied input vectors and<br />

the sequence in which the input vectors are applied, the power consumption due to the internal nodes<br />

of logic gates may contribute a significant portion of the total power consumption. Experimental results<br />

in section 20.5 show that the power consumption due to the internal nodes can be as high as 20% of the<br />

total power consumption for some circuits.<br />

The impact of the internal nodes in the total power consumption is most significant when the internal<br />

nodes are switching, but the output node remains unchanged, as shown in Fig. 20.4. The internal<br />

capacitance, Cinternal,<br />

is being charged, discharged, and recharged at time t0,<br />

t1,<br />

and t2,<br />

respectively. During<br />

this period of time, power is dissipated solely due to charging and discharging of the internal node.<br />

FIGURE 20.4<br />

P total<br />

1<br />

2<br />

-- ⋅ Cload ⋅ Vsupply ⋅<br />

2<br />

1 2<br />

-- ⋅ Vsupply ⋅<br />

2<br />

Charging and discharging of internal node.<br />

B<br />

=<br />

n<br />

∑<br />

i=1<br />

A B<br />

A<br />

2-input NAND<br />

V dd<br />

A+ Iavg ⋅ Vsupply + Ileakage ⋅ Vsupply C load i<br />

⋅<br />

A i<br />

H = Logic High<br />

Vout L = Logic Low<br />

C-load<br />

t0 , t2 t0 t1 t2 A : H L H<br />

Vint B : L H L<br />

V<br />

C-int<br />

out : H H H<br />

Vint : H L H<br />

t1

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