All of the commonly available permanent magnet materials experience either reversible or permanent changes in magnetic output as a result of exposure to temperatures above or below room temperature.
Changes in temperature affect both flux output, which is proportional to Br, and resistance to demagnetization, which is proportional to Hci. The magnitude of these change are related to the reversible temperature coefficient of induction (Br) or the reversible temperature coefficient of coercivity (Hci). These are referred to as α (alpha) for Br and β (beta)for Hci respectively. The table below shows the temperature coefficients for a range of magnet types:
Material |
Grade |
Alpha (%/C°) |
Beta (%/C°) |
Curie Temperature (C°) |
Alnico | 5 | -0.02 | -0.01 | 900 |
Alnico | 8 | -0.02 | -0.01 | 860 |
Sm2Co5 | 20 MGOe | -0.04 | -0.4 | 700 |
Sm2Co17 | 27 MGOe | -0.035 | -0.2 | 810 |
Bonded NdFeB | MQP-A | -0.13 | -0.4 | 312 |
Bonded NdFeB | MQP-B | -0.11 | -0.4 | 360 |
Sintered NdFeB | N48M | -0.12 | -0.65 | 312 |
Sintered NdFeB | N38SH | -0.12 | -0.65 | 312 |
Sintered NdFeB | N38UH | -0.1 | -0.55 | 340 |
Hard Ferrite | C5, C8 | -0.2 | 0.27 | 450 |
There are three types of loss in magnetic output influenced by the above temperature coefficients and the Curie temperature of the magnet. These are defined as follows:
Because of the variation in the temperature coefficients and Curie temperatures different permanent magnet materials and grades have a wide range of working temperatures. The table below lists the various materials and their suggested maximum working temperatures:
Interesting fact: Because the temperature coefficient of Br for Sm2Co17is significantly lower than that of NdFeB that around 150 C° and above a Sm2Co17 magnet outperforms NdFeB in terms of its (BH)max.