Summarizing Inductance
Summary
- Inductance is the property of a device that tells how effectively it induces an emf in another device.
- Mutual inductance is the effect of two devices in inducing emfs in each other.
- A change in current \(\Delta {I}_{1}/\Delta t\) in one induces an emf \({\text{emf}}_{2}\) in the second:
\({\text{emf}}_{2}=-M\cfrac{\Delta {I}_{1}}{\Delta t}\text{,}\)
where \(M\) is defined to be the mutual inductance between the two devices, and the minus sign is due to Lenz’s law. - Symmetrically, a change in current \(\Delta {I}_{2}/\Delta t\) through the second device induces an emf \({\text{emf}}_{1}\) in the first:
\({\text{emf}}_{1}=-M\cfrac{\Delta {I}_{2}}{\Delta t}\text{,}\)
where \(M\) is the same mutual inductance as in the reverse process. - Current changes in a device induce an emf in the device itself.
- Self-inductance is the effect of the device inducing emf in itself.
- The device is called an inductor, and the emf induced in it by a change in current through it is
\(\text{emf}=-L\cfrac{\Delta I}{\Delta t}\text{,}\)
where \(L\) is the self-inductance of the inductor, and \(\Delta I/\Delta t\) is the rate of change of current through it. The minus sign indicates that emf opposes the change in current, as required by Lenz’s law. - The unit of self- and mutual inductance is the henry (H), where \(1 H=1 \Omega \cdot \text{s}\).
- The self-inductance \(L\) of an inductor is proportional to how much flux changes with current. For an \(N\)-turn inductor,
\(L=N\cfrac{\Delta \Phi }{\Delta I}\text{.}\)
- The self-inductance of a solenoid is
\(L=\cfrac{{\mu }_{0}{N}^{2}A}{\ell }\text{(solenoid),}\)
where \(N\) is its number of turns in the solenoid, \(A\) is its cross-sectional area, \(\ell \) is its length, and \({\text{μ}}_{0}=4\pi ×{\text{10}}^{\text{−7}}\phantom{\rule{0.25em}{0ex}}\text{T}\cdot \text{m/A}\phantom{\rule{0.10em}{0ex}}\) is the permeability of free space. - The energy stored in an inductor \({E}_{\text{ind}}\) is
\({E}_{\text{ind}}=\cfrac{1}{2}{\text{LI}}^{2}\text{.}\)
Glossary
inductance
a property of a device describing how efficient it is at inducing emf in another device
mutual inductance
how effective a pair of devices are at inducing emfs in each other
henry
the unit of inductance; \(1\phantom{\rule{0.25em}{0ex}}\text{H}=1\phantom{\rule{0.25em}{0ex}}\Omega \cdot \text{s}\)
self-inductance
how effective a device is at inducing emf in itself
inductor
a device that exhibits significant self-inductance
energy stored in an inductor
self-explanatory; calculated by \({E}_{\text{ind}}=\cfrac{1}{2}{\text{LI}}^{2}\)
This lesson is part of:
Electromagnetic Induction and AC Circuits