Module 4 : Propagation Delays in MOS
Lecture 19 : Analyzing Delay for various Logic Circuits
 
Contd...
The previous equation for Vx(t) can be solved as-
The variation of the node voltage Vx(t)is plotted as a function of time in fig. 19.22. The voltage rises from its initial value of 0 and reaches Vmax =VDD-Vtn after a large time. The pass transistor will turn off when Vx = Vmax. Since Vgs= Vtn. Therefore Vx can never attain VDD during logic 1 transfer. Thus we can use buffering to overcome this problem.
Logic “0” Transfer: Assume that the Vx=1 initially. A logic“0” level is
Fig 19.22: Node Voltage Vx vs t
applied to the input terminal which corresponds to Vin=1. Now the clock signal at the gate of the pass transistor goes from 0 to VDD at t=0. It can be seen that the pass transistor starts to conduct and operate in linear mode throughout this cycle and the drain current flows in the opposite direction to that of charge up.
Analysis: We can write -
The above equation for Vx(t) can be solved as -
Plot of Vx(t) is shown in figure 19.23.
 
Fig 19.22: Node Voltage Vx vs t
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
4