## Why we have been wrong about ‘magnetic field strength’

The British Institute of Radiology recently published three information sheets on MRI safety. Myths and maths was one of them. In this series I’d like to expand on themes of that sheet. More details can be sourced from my book Essentials of MRI Safety.

Myth: the tesla is the SI unit of magnetic field strength

Maths: the tesla is the SI unit of magnetic flux density. Magnetic field strength or intensity is measured in amperes per metre. We have been using the wrong terminology for decades!

BIR Information Sheet

We’ve all said it: “What field strength is your scanner?”

Correct answer: approximately 1.2 million amperes/metre (1,193,662 A/m).

Why is this? Because ‘magnetic field strength’ or intensity (denoted H) is a different physical quantity. What we incorrectly refer to as ‘field strength’ is actually magnetic flux density (B).

### Does it matter?

In a vacuum or in air – no. B and H are related through a constant μ0 (= 4π x 10-7 henrys per metre – H/m).

In a magnetic medium- yes it matters very much. You can think of it in this way. The H-field is produced when you have a current (amps) flowing through a coil. So the scanner produces an H-field. The B-field is what you get within a medium. In the case of air B =μ0H, but in another medium the flux density is the sum of the field arising from induction (the H-field) plus the field arising from magnetisation of the material.

Considering ferromagnetic metals, we talk about the ‘saturation B-field.’ This is incorrect and misleading. B does not saturate. It is the magnetisation M (also measured in A/m) that saturates. Above saturation, B will continue to increase as H is increases, e.g. by moving the object closer to the scanner (although this will probably result in a projectile accident- so don’t try it).

It’s misleading to think of a ‘saturation B value’ or Bsat because the simplistic and wrong implication is that the object will magnetically saturate in an external field equal to Bsat, whereas the truth is that it will saturate in a much smaller external field- further away from the bore opening – and highly dependent upon the shape of the object.

Another cause of confusion that arises from our misuse of ‘field strength’ lies with the expressions we use to calculate the translational (projectile) force on objects. We see in the literature (including Essentials of MRI Safety) complicated equations involving the B-field and its spatial gradient but differing for para/dia magnetic and saturated/unsaturated ferromagnetic objects. These are not wrong, but the direct cause of the translational force is not magnetic flux density B, but the magnetisation Mz of the object as well as the spatial gradient of the B-field. More simply the force is always (for all materials):

V is the volume of the object, dB/dz the spatial gradient of the external B-field. Of course the value of M does depend upon B (and H) but it’s the interaction of M with dB/dz that propels the object. As explained in Myths and Maths 1, it is magnetisation which is the key factor for the translational force.

### So what is B?

To answer that let’s turn to the definition of its unit, the tesla (T). 1 T is defined as being the magnetic flux density required to produce a force of 1 newton (N) on an electrical charge of 1 coulomb (C) moving perpendicular to the B-field with a velocity of 1 metre per second (m/s).