Dis/Charging capacitor in time varying electric field

AI Thread Summary
The discussion focuses on calculating capacitive current in a capacitor subjected to a time-varying electric field, specifically when the electric field is represented by a random function, which complicates the use of the standard formula for capacitive current. The user seeks to determine the charge q(t) on a capacitor in an RC circuit with a step function voltage applied in three intervals, with specific voltage values for each interval. They have successfully calculated q(t) for the second interval but are struggling to derive it for the third interval, where the voltage decreases. Another participant suggests maintaining the charge from the end of the second interval as a reference for calculations in the third interval, emphasizing the capacitor's ability to retain charge based on previous voltages and time intervals. The conversation highlights the complexities of analyzing capacitors in non-static electric fields.
Apteronotus
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I'm interested in calculating the capacitive current when the electric field across a capacitor is given by a random function. The randomness of the electric field deems the usual I_c=C\frac{dV}{dt} useless; since the derivative of a random function V cannot be calculated.

To approach the problem in another way, I'd like to calculate the charge q(t) on a capacitor in an RC circuit when the emf is given by a step function:
V(t)=V_1 for t\in(0,t_1)
V(t)=V_2 for t\in(t_1,t_2)
and
V(t)=V_3 for t\in(t_2,t_3)
where
V_1<V_3<V_2
I've calculated the charge q(t) for t\in(t_1,t_2) to be
q(t)=q_1+C(V_2-V1)(1-e^{\frac{t_1-t}{RC}})
but am having a difficult time deriving the charge in the interval (t_2,t_3).

If anyone can help me with either of the problems I'd much appreciate it.

Thanks.
 
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Apteronotus said:
I'm interested in calculating the capacitive current when the electric field across a capacitor is given by a random function. The randomness of the electric field deems the usual I_c=C\frac{dV}{dt} useless; since the derivative of a random function V cannot be calculated.

To approach the problem in another way, I'd like to calculate the charge q(t) on a capacitor in an RC circuit when the emf is given by a step function:
V(t)=V_1 for t\in(0,t_1)
V(t)=V_2 for t\in(t_1,t_2)
and
V(t)=V_3 for t\in(t_2,t_3)
where
V_1<V_3<V_2
I've calculated the charge q(t) for t\in(t_1,t_2) to be
q(t)=q_1+C(V_2-V1)(1-e^{\frac{t_1-t}{RC}})
but am having a difficult time deriving the charge in the interval (t_2,t_3).

If anyone can help me with either of the problems I'd much appreciate it.

Thanks.

I'm not understanding the setup yet. The electric field between the plates is determined by the plate voltage difference. Are you suggesting somehow to change that?
 
Hi Berkeman,

Lets simply suppose we have an RC circuit connected to a voltage device (battery).
For the first time interval (0,t_1) the battery voltage is V_1 for the second interval (t_1,t_2) the voltage is V_2 and so on...

I want to measure the the amount of charge that would accumulate on the capacitor as a function of time.

For the first time interval, we simply have
q(t)=CV_1(1-e^{-\frac{t}{RC}})
for the second time interval we'd get
q(t)=CV_1(1-e^{-\frac{t_1}{RC}}) + C(V_2-V_1)(1-e^{-\frac{t_1-t}{RC}})

now considering that V_3<V_2 the capacitor need to discharge slightly.
So what is q(t) in the third time interval?

Thanks.
 
Apteronotus said:
Hi Berkeman,

Lets simply suppose we have an RC circuit connected to a voltage device (battery).
For the first time interval (0,t_1) the battery voltage is V_1 for the second interval (t_1,t_2) the voltage is V_2 and so on...

I want to measure the the amount of charge that would accumulate on the capacitor as a function of time.

For the first time interval, we simply have
q(t)=CV_1(1-e^{-\frac{t}{RC}})
for the second time interval we'd get
q(t)=CV_1(1-e^{-\frac{t_1}{RC}}) + C(V_2-V_1)(1-e^{-\frac{t_1-t}{RC}})

now considering that V_3<V_2 the capacitor need to discharge slightly.
So what is q(t) in the third time interval?

Thanks.

It looks like you are on the right track. Just do what you did fror the 2nd equation. Fix the 2nd term at t2 to make hold whatever it was at at the end of t2, and write a similar 3rd equation with the voltage difference with respect to that fixed 2nd term. The capacitor sort of has "memory" in that it is storing some amount of charge, based on its past histopry and the Vn voltages and tn time intervals.
 
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