Express current in time and frequency domain (capacitor)

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The discussion focuses on calculating the current through a capacitor given specific voltage inputs in both time and frequency domains. For the first voltage input, the current is derived as I(t) = 3.77 cos(ωt + 60°) mA, with the corresponding phasor representation of 3.77 mA ∠60°. For the second voltage input, the current is calculated as I(t) = 4.524 sin(377t + 150°) A, leading to the phasor I = 4.524 mA ∠150°. The conversation emphasizes the importance of matching the trigonometric functions for consistency in phase reference. The use of complex numbers for phasor calculations is also recommended for simplifying the process.
Color_of_Cyan
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Homework Statement




Calculate the current in the capacitor shown if the voltage input is

a. v1(t) = 10cos(377t - 30°)V
b. v2(t) = 12sin(377t + 60°)V




Give answers in both time and frequency domain.



Homework Equations



I = dQ/dt = C * dV/dt


The Attempt at a Solution



I = dQ/dt = C * dV/dt

I = 1ρF * (d/dt)(10 * cos(377t - 30°)v

Took derivative:

I(t) = 1μF * (-3770 * sin(377t - 30°)

I(t) = (-3.77 x 10-3)(sin(377t - 30°))A


If the above is correct, where can I start with converting this to frequency domain though? I know it's supposed to be something like in form e^t.
 
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What you've done so far is fine. You've got the current expressed as a sine function, while the starting point was a voltage expressed as a cosine function. You may find that, sometimes, it is desirable to express the result using the same trig function as you began with (i.e., then both current and voltage time domain functions use the same trig function).

For the frequency domain you'll be working with phasors. Have you covered them?
 
So ω = 377 and the phasor current for that looks to be

I = (-3.77 x 10-3)∠-30° ? Would that be it?
 
Color_of_Cyan said:
So ω = 377 and the phasor current for that looks to be

I = (-3.77 x 10-3)∠-30° ? Would that be it?

Sure. But usually the magnitude of a phasor is a positive value. You can normalize the phasor by folding the negation into the angle.

And, if you want to place the current phasor on the same reference axes as the voltage phasor (so that the "PHASE" part of phasor is actually useful), you should first convert the current's sine to cosine so the trig function matches that of the driving voltage. Then the phase angles will be referenced to the same starting point.

So, the steps are:

i(t) = -3.77 sin(ωt - 30°) mA
i(t) = 3.77 sin(ωt - 30° + 180°) mA
i(t) = 3.77 cos(ωt - 30° + 180° - 90°) mA

So:

i(t) = 3.77 cos(ωt + 60°) mA

and your phasor is 3.77 mA ∠60

I see that for part (b) the trig function in the time-domain voltage is sine, so you'll want to manipulate the current's expression to be likewise.

Personally I find it easier to employ complex numbers to work with phasors and impedance in the frequency domain. Then essentially all the angle offsets are handled automatically by the complex arithmetic :wink:
 
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So is the second current:

I = (4.524 x 10-3)(sin(377t + 150°)A ?

Then the phasor

I = 4.524 mA ∠ 150° ?
 
Looks good!
 
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