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In the circuit, shown below, if the values of R and C are very large, the form of the
output voltage for a very high frequency square wave input, is best represented by





Step 1: Understanding the Square Wave Input
The input voltage
is a square wave defined as:
This pattern repeats every T seconds.
Step 2: Charging Phase (
)
At t=0, the source switches to +1V, and the capacitor begins charging from its initial voltage
(where
).
The charging equation for the capacitor voltage is:
Here:
= +1V (target voltage).
(starting voltage).
Substituting these values:
At
, the capacitor voltage reaches +V (due to steady-state symmetry):
Step 3: Solving for V
Rearranging the equation:
For high RC(
) , the exponential term can be approximated using the Taylor series:
Substituting this approximation:
Simplifying:
Neglecting the small term
:
The exact solution is:
For
, so
.
Step 4: Discharging Phase 
At
, the source switches to
, and the capacitor begins discharging toward
from
.
The discharging equation is:
At
, the capacitor voltage reaches
, completing the cycle.
Final Expression for Capacitor Voltage
For
:
For
:
Conclusion
The capacitor voltage
oscillates between
and
, where:

This is because the capacitor cannot fully charge/discharge due to the high RC time constant. The waveform resembles a clipped exponential curve, oscillating below the input square wave amplitude.