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energy stored in an inductor |
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| Nov5-09, 07:38 AM | #1 |
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energy stored in an inductor
so the amount of work done to drive the current through the inductor is given by
dw=Eidt where E is the emf of the variable voltage source.We put E=+L (di/dt). can you please tell me why we put that value?? (i know the induced e.m.f on the inductor is - L (di/dt) thanks
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| Nov5-09, 09:32 AM | #2 |
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Recognitions:
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while calculating the amount of work done we have to take the integration. For that we have to reduce the expression of dw in single variable
So dw = Eidt = L*i*di/dt*dt = L*i*di. Now take integrations to get the energy stored in the inductor. |
| Nov6-09, 05:23 AM | #3 |
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| Nov6-09, 08:19 PM | #4 |
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energy stored in an inductorThe reason why it's positive for your given equation, is because positive work must be done to induce the current. We need only the magnitude of E then. |
| Nov8-09, 04:24 AM | #5 |
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but why to drive the current through the circuit so as to defeat the induced e.m.f -L di/dt we need Ldi/dt; dont we not need a greater value??thanks again. |
| Nov8-09, 04:38 AM | #6 |
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Recognitions:
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The induced emf is Ldi/dt; the negative sign just indicates it opposes the battery's emf. The electrons pushed through the inductor must overcome a voltage of Ldi/dt (that is, they must overcome an increase in potential of magnitude Ldi/dt), so they gain Lidi/dt of potential energy per unit time. This gain in potential is what the energy stored in the inductor really is.
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| Nov8-09, 08:29 AM | #7 |
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Consider a circuit with an applied emf, resistor, and inductor, where the current varies with time. If the current is increasing (di/dt > 0 ), then the self-induced emf opposes the direction of the applied emf. If the current is decreasing (di/dt < 0), the self-induced emf is actually oriented in the same direction as the applied emf. In both cases, the self-induced emf has orientation that always opposes the "change in current", not the "applied emf." |
| Nov13-09, 08:27 AM | #8 |
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thanks :-)
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