The search coil magnetometer or induction magnetometer, based on an inductive sensor (also known as inductive loop and inductive coil), is a magnetometer which measures the varying magnetic flux. An inductive sensor connected to a conditioning electronic circuit constitutes a search coil magnetometer. It is a vector magnetometer which can measure one or more components of the magnetic field. A classical configuration uses three orthogonal inductive sensors. The search-coil magnetometer can measure magnetic field from mHz up to hundreds of MHz.
Principle The inductive sensor is based on Faraday's law of induction. The temporal variation of the magnetic flux Φ {\displaystyle \Phi } through a N turns circuit will induce a voltage e {\displaystyle e} which follows
e = − N d Φ d t {\displaystyle e=-N{\frac {\mathrm {d} \Phi }{\mathrm {d} t}}}
which can be expressed in a simpler way
e = − N S d B d t {\displaystyle e=-NS{\frac {\mathrm {d} B}{\mathrm {d} t}}}
by assuming that the induced magnetic field B is homogeneous over a surface S (the magnetic flux will be expressed Φ = B × S {\displaystyle \Phi =B\times S} ).
The induced voltage ( e {\displaystyle e} ) may be increased several ways:
increase the surface (S), increase the turn number (N), use a ferromagnetic core.
Search coil using a ferromagnetic core When a coil is wound around a ferromagnetic core, that increases the sensitivity of the sensor thanks to the apparent permeability of the ferromagnetic core.
Apparent permeability The magnetic amplification, known as apparent permeability μ a p p {\displaystyle \mu _{app}} , is the result of the magnetization of the ferromagnetic core response to an external magnetic field. The magnetization is reduced by the demagnetizing field.
μ a p p = μ r 1 + N z ( μ r − 1 ) {\displaystyle \mu _{app}={\frac {\mu _{r}}{1+N_{z}(\mu _{r}-1)}}}
where μ r {\displaystyle \mu _{r}} is the relative permeability, N z {\displaystyle N_{z}} is the demagnetizing coefficient in the z direction. The induced voltage will be written
− N e = N S μ a p p N d B d t {\displaystyle -Ne=NS\mu _{app}{\frac {N\mathrm {d} B}{\mathrm {d} t}}}
The demagnetizing coefficient can easily be computed in the case of simple shapes (spheres and ellipsoids).
Applications Eye tracker § Eye-attached tracking Non-destructive testing Magnetotellurics Space research
References
See also Waves (Juno) (Uses a magnetic search coil)
