Question about this Capacitor voltage integral equation

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SUMMARY

The discussion clarifies the derivation of the capacitor voltage equation, specifically transitioning from the integral form v(t) = 1/C ∫t-∞ i(τ) dτ to v(t) = 1/C ∫tt0 i(τ) dτ + v(t0). The key concept is recognizing that the initial voltage v(t0) acts as a constant representing the capacitor's initial condition. This understanding allows for the separation of the integral into two parts, effectively capturing the history of current flow through the capacitor.

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JMFernandez
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Hi.

I don´t know if this question should be in the maths forum, but as it´s related with circuit analysis, I will post it here. I just would like to know how you get:

v(t) = 1/C ∫tt0 i(τ) dτ + v(t0)

From:

v(t)=1/C ∫t-∞ i(τ) dτ

I just know the basics of calculus and I don´t know how to operate the second equation to get the first one.

Thank you in advance.
 
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JMFernandez said:
Hi.

I don´t know if this question should be in the maths forum, but as it´s related with circuit analysis, I will post it here. I just would like to know how you get:

v(t) = 1/C ∫tt0 i(τ) dτ + v(t0)

From:

v(t)=1/C ∫t-∞ i(τ) dτ

I just know the basics of calculus and I don´t know how to operate the second equation to get the first one.

Thank you in advance.
The equation describes how the cap voltage changes as current flows through it. Fortunately, all of the history of past current flow(s) is represented by the voltage at any time. That is what the initial voltage ##v(t_o)## is. Since that doesn't depend on the variable ##t##, we can just call it a constant value, the "initial condition" of the capacitor. So,

$$v(t) = \frac{1}{C} \int_{-∞}^{t} i(\tau) \, d\tau = \frac{1}{C} \int_{-∞}^{t_o} i(\tau) \, d\tau + \frac{1}{C} \int_{t_o}^{t} i(\tau) \, d\tau \equiv v(t_o) + \frac{1}{C} \int_{t_o}^{t} i(\tau) \, d\tau$$
 
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Thank you. Very clear and concise explanation!!
:smile::smile:
 
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