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An electrical generator converts mechanical work into electrical energy. In an induction generator, relative motion changes how a conducting circuit interacts with a magnetic field. For an ideal coil with $N$ turns and area $A$, rotating at angular velocity $\omega$ in a uniform field of magnitude $B$, the linked magnetic flux is $NBA\cos \omega t$. Faraday's law gives the electromotive forcewith sign determined by the chosen loop orientation. Connecting a load lets this electromotive force drive an electric current; the resulting electromagnetic torque opposes the driving motion, consistent with conservation of energy.

Michael Faraday's rotating-disc apparatus makes the conversion visible without a many-turn coil. A copper disc rotated between magnetic poles, with an external circuit contacting its axle and rim. The motion-dependent Lorentz force separates charge between those contacts. This homopolar generator maintains one output polarity for a fixed field and rotation direction, unlike the alternating output of the rotating-coil example.^[ref]

An original quantitative demonstration compares the open-circuit output at different rotation rates while retaining the same coil and field geometry. The ideal prediction is proportionality to $\omega$. Under load, losses and the required driving torque supply additional tests of the conversion model.

Connect a homopolar generator to a solenoid producing its own axial field. Reinforcing winding and rotation give $C={\mu }_{0}N{a}^2/(2l)$ and $L\dot{I}=(C\omega -R)I$. A seed field grows for $\omega >R/C$, is marginal at equality, and decays below threshold. An identically zero initial field remains zero in this homogeneous ideal model; startup requires a seed or perturbation.

Self-inductance relates current to its own magnetic flux linkage: $\Lambda =LI$, so the induced electromotive force is $-L\dot{I}$ for fixed geometry. A long solenoid has $B={\mu }_{0}NI/l$ and area $\pi a^2$. Its $N$ turns giveThe homopolar generator uses a disc rotating through this axial field; integrate the motional Lorentz force from shaft to rim:For a homopolar disc dynamo, choose the wiring and rotation sense giving positive magnetic feedback. Kirchhoff's voltage law isfor prescribed constant $\omega$. ThusA nonzero seed grows when $\omega >{\omega }_c$, decays when $\omega <{\omega }_c$, and is marginal at equality. This explains the printed $\omega \ge {\omega }_c$ as the threshold including its boundary; equality does not itself give exponential growth. An exactly zero initial current remains zero in the ideal homogeneous equation, and reversing the feedback sense prevents the instability.

In the torque-controlled homopolar dynamo equilibrium, a radial current element exerts a braking torque $d{G}_B=IBrdr$, so $G_B=IB{a}^2/2=C{I}^2$. For steady rotation and nonzero steady current, $G=C{I}^2$ and $\omega ={\omega }_c$. Hence the field intensity magnitude isThe two current signs give opposite magnetic polarities. Finally,The steady magnetic and rotational energies do not change. This is a steady-state balance, not an assertion that every dynamical trajectory must approach that state.