MCQ
Average energy stored in a pure inductance $L$ when a current $i$ flows through it, is
- A$L{i^2}$
- B$2L{i^2}$
- C$\frac{{L{i^2}}}{4}$
- ✓$\frac{{L{i^2}}}{2}$
Work done against back $e.m.f$. $e$ in time dt and current i is
$dW = - eidt = L\frac{{di}}{{dt}}idt = Li\;di$ $ \Rightarrow \;W = L\int_0^i {i\;di} = \frac{1}{2}L{i^2}$
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$(A)$ They will never come out of the magnetic field region.
$(B)$ They will come out travelling along parallel paths.
$(C)$ They will come out at the same time.
$(D)$ They will come out at different times.
| LIST-I | LIST-II | ||
| A. | Gravitational constant | I. | [LT^(-2)] |
| B. | Gravitational potential energy | II. | [L^(2)T^(-2)] |
| C. | Gravitational potential | III. | [ML^(2)T^(-2)] |
| D. | Acceleration due to gravity | IV. | [M^(-1)L^(3)T^(-2)] |