Maxwell coil

A Maxwell coil is a device for producing a large volume of almost constant (or constant-gradient) magnetic field. It is named in honour of the Scottish physicist James Clerk Maxwell.

Magnetic field lines around a Maxwell coil
Modulus of the magnetic field around a Maxwell coil

A Maxwell coil is an improvement of a Helmholtz coil: in operation it provides an even more uniform magnetic field (than a Helmholtz coil), but at the expense of more material and complexity.

Description

A constant-field Maxwell coil set consists of three coils oriented on the surface of a virtual sphere.[1]
According to Maxwell's original 1873 design:[2]
each of the outer coils should be of radius , and distance from the plane of
the central coil of radius .
The number of ampere-turns of each of the smaller coils should equal exactly of the middle coil.
This arrangement removes variations in magnetic field, up to its 6th-order derivative with respect to position, near the centre of the virtual sphere.
If using a single current source, a possible ratio of windings is 64 for the central coil and 49 for the outer coils, as famously represented in Maxwell's original 1873 design.
This ratio of 49/64 is approximately 101.28 percent of .
Another, more precise ratio of windings is 86 for the central coil and 65 for the outer coils, which is approximately 100.015 percent of .
Additionally, a 37/49 ratio, which is more economical than the 49/64 design, yields a 100.1095 percent of the ideal .
Finally, a simple ratio of 3/4, results in a shocking 100.79 percent of the ideal ratio. This means that if Maxwell were to have used 48 instead of 49 windings on the outer coils of his original 1873 proposed design, this 48/64 (or 3/4) design would have had nearly a 0.5% improved field contribution by these outer windings.

Gradient-field Maxwell coil

A gradient-field Maxwell coil is essentially the same geometry of the 3-coil configuration above, with the central coil removed to leave only the smaller two coils.[3] If the current in one of the coils is reversed, a uniform-gradient magnetic field is produced near the centre of the two coils. Maxwell describes the use of the 2-coil configuration for the generation of a uniform force on a small test coil.[4] A Maxwell coil of this type is similar to a Helmholtz coil with the coil distance increased from coil radius to and the coils fed with opposite currents.

See also

References
  1. Garrett, Milan Wayne (1967). "Thick Cylindrical Coil Systems for Strong Magnetic Fields with Field or Gradient Homogeneities of the 6th to 20th Order". Journal of Applied Physics. 38 (6): 2563–2586. Bibcode:1967JAP....38.2563G. doi:10.1063/1.1709950.
  2. Clerk-Maxwell, James (1873). Treatise on Electricity and Magnetism. 2. Oxford: The Clarendon Press. p. 319. ISBN 978-0-486-60636-1.
  3. R. Pascone, Manhattan College, T. Vullo and P.T. Cahill (1993) Theoretical and experimental analysis of magnetic field gradients for MRI from IEEE Explore
  4. Clerk-Maxwell, James (1873). Treatise on Electricity and Magnetism. 2. Oxford: The Clarendon Press. p. 333. ISBN 978-0-486-60636-1.
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