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Q62PE

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Found in: Page 862

College Physics (Urone)

Book edition 1st Edition
Author(s) Paul Peter Urone
Pages 1272 pages
ISBN 9781938168000

(a) Calculate the self-inductance of a $${\rm{50}}{\rm{.0}}$$cm long, $${\rm{10}}{\rm{.0}}$$cm diameter solenoid having $${\rm{1000}}$$ loops. (b) How much energy is stored in this inductor when $${\rm{20}}{\rm{.0}}$$ A of current flows through it? (c) How fast can it be turned off if the induced emf cannot exceed $${\rm{3}}{\rm{.00}}$$V?

(a.) The inductor's self-inductance is $${\rm{19}}{\rm{.7mH}}$$.

(b.) The inductor has $${\rm{3}}{\rm{.95\;J}}$$ of energy stored in it.

(c.) The shortest time in which the emf will be less than $$3\;{\rm{V}}$$ is $${\rm{131\;ms}}{\rm{.}}$$

See the step by step solution

Step 1: Information Provided

• Length of the coil: $$l = 50.0\;{\rm{cm}}$$.
• Diameter of the coil: $$d = 10.0\;{\rm{cm}}$$.
• Number of loops: $$N = 1000$$
• Current flowing through the inductor coil: $$\Delta I = 20.0 {\rm{A}}$$.
• Maximum Induced emf: $$\varepsilon = \;3.0\;{\rm{V}}$$

Step 2: Concept Introduction

If a solenoid is connected to an A.C. source, due to the continuously changing magnetic field produced by the solenoid, an emf is induced in the same solenoid. This induced emf is such that it opposes the change in the magnetic field. This phenomenon is called self-inductance.

Step 3: Calculating Self-Inductance and Force

a)

The inductor's self-inductance is calculated as

$$L = \frac{{{\mu _0}{N^2}A}}{l}$$

where $$A = \frac{{\pi {D^2}}}{4}$$is the cross-section area, $$N$$ is the number of turns, and $$l$$ is the coil length. As a result, we will have-

\begin{aligned} L &= \frac{{\pi {\mu _0}{N^2}{D^2}}}{{4l}}\\ &= \frac{{\pi \times \left( {4\pi \times {{10}^7}\;{\rm{H}}{{\rm{m}}^{{\rm{ - 1}}}}} \right) \times {{1000}^2} \times {{\left( {0.1\;{\rm{m}}} \right)}^2}}}{{4 \times \left( {0.5\;{\rm{m}}\;} \right)}}\\ &= 1.97 \times {10^{ - 2}}\;{\rm{H}}\end{aligned}

Therefore, the self-inductance of the solenoid is $$1.97 \times {10^{ - 2}}\;{\rm{H}}$$

Step 4: Calculating Stored Energy

b)

When the inductance and current are known, the energy stored in an inductor is given by

$$E = \frac{{L{I^2}}}{2}$$

Numerically in our case we will have

\begin{aligned} {\rm{E }}&=\frac{{\left( {{\rm{0}}{\rm{.0197}}\;{\rm{H}}} \right){\rm{ \times }}{{\left( {{\rm{20}}\;{\rm{A}}} \right)}^{\rm{2}}}}}{{\rm{2}}}\\{\rm{ }}&={\rm{.94\;J}}\end{aligned}

Therefore, energy stored in the inductor is $${\rm{3}}{\rm{.94\;J}}$$

Step 5: Calculating induced electromotive force

c)

if we ignore the sign, the induced electromotive force is given as-

$$\varepsilon = \frac{{L\Delta I}}{{\Delta t}}$$

the shortest time$$\Delta t$$ for the emf not to surpass a given amount $$\varepsilon$$ is-

$$\Delta t = \frac{{L\Delta I}}{\varepsilon }.$$

Numerically, we will have

\begin{aligned} \Delta t &= \frac{{0.0197\;{\rm{H}} \times 20\;{\rm{A}}}}{{3\;{\rm{V}}}}\\ &= 0.13\;{\rm{s}}\end{aligned}

Therefore, the shortest time in which the emf will not exceed $$3\;{\rm{V}}$$ is $${\rm{0}}{\rm{.131\;s}}$$.