Herzenberg dynamo
Builds on Dynamo theoryMagnetohydrodynamicsBullard disc dynamo
Statement
Let a large sphere of uniform electrical conductivity be surrounded by an insulator. Let it contain two small rigid spheres of radius made of the same conductor, in perfect electrical contact with it. Let the distance between their centres satisfy . Let each small sphere rotate rigidly with angular speed about an axis through its centre. Let the rest of the conductor stay at rest. Consider the magnetic induction equation of magnetohydrodynamics with this velocity field. For suitable non-parallel orientations of the two axes and for above a critical value, it has a solution with a non-decaying magnetic field. So kinematic dynamo action is possible in a body of uniform conductivity.
Remarks
Herzenberg published this example in 1958; in the same year Backus gave another rigorous example with a time-dependent flow. These were the first rigorous existence proofs for homogeneous kinematic dynamos. They answered the doubt raised by Cowling's antidynamo theorem, which rules out axisymmetric dynamos. The proof uses . Near each sphere, the field is computed as the response of that sphere to the nearly uniform field produced there by the other sphere. Then a self-consistent pair of responses is sought. The arrangement is chiral; if the two axes are parallel, the mutual reinforcement fails.
Going deeper
For a student
In dynamo theory the kinematic problem fixes the flow and asks whether the induction equation has growing or steady solutions. Antidynamo theorems show that flows that are too symmetric fail. The Herzenberg dynamo is a carefully chosen asymmetric flow for which the answer can be computed by asymptotic analysis. It is an analogue of the Bullard disc dynamo in a body of uniform conductivity, with no insulating wires to direct the current.
Reading path
To understand this page from the ground up, read these 5 pages in order. The foundations come first.
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- no evidence level
- Dynamo theory concept
- Exponential function concept
- Magnetohydrodynamics concept
- Bullard disc dynamo example
- Herzenberg dynamo statement
Further reading
About this page
| Tag | MNP5AZJZ4H |
|---|---|
| URI | m2://MNP5AZJZ4H |
| Kind | statement, theorem |
| Writing | W0 stub |
| MSC | 76W05, 86A25 |
| Status | This copy of the site has no build data. Run m2 status MNP5AZJZ4H. |
| About | Dynamo theory |
| Uses | Dynamo theory, Magnetohydrodynamics, Bullard disc dynamo |
| Changed | 3 November 2026 |
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