Electromagnet heat source and efficiency

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SUMMARY

The discussion focuses on the efficiency of electromagnets used in biomedical applications, particularly regarding heat generation. The primary source of heat is identified as winding losses, calculated using the formula P=I^2 R, where reducing current can mitigate these losses but may decrease magnetic flux density. Core losses, associated with the ferromagnetic material of the electromagnet, also contribute to heat but are less significant when using DC excitation. Strategies to enhance efficiency include optimizing winding materials and configurations to balance current and resistance while maintaining magnetic flux density.

PREREQUISITES
  • Understanding of electromagnet principles and operation
  • Familiarity with electrical resistance and power loss calculations
  • Knowledge of ferromagnetic materials and their properties
  • Basic concepts of AC and DC current applications
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Biomedical engineers, electrical engineers, and researchers focused on improving electromagnet efficiency and heat management in medical applications.

anorred
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So.. I'm a biomedical engineer, and a new technology that is arising is being able to control magnets that "swim" around the body using electromagnets oriented around the outside of the patients body. It has been said that electromagnets can't be used on the inside of the patient because they get too hot.

What is the source of the majority of the heat? Is it the current moving through the wire, or the current induced in the core of the electromagnet?

Are there methods to make electromagnets more efficient to reduce heat?
 
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In a electromagnet one can basically divide the power losses into two categories, winding losses and core losses.

Winding losses are caused by the current flowing in the coil/winding of the electromagnet. These losses are equal to : P=I^2 R, where I is the current, and R is the resistance of the winding. To reduce the winding losses, the most effective method, due to the ^2 term, is to reduce the current. This again may reduce the magnetic flux density produced.
Or one can change the resistivity of the winding by changing the material (copper, aluminium etc.) or the length/number of turns of the winding. The latter also reduces the magnetic flux density.

Since the magnetic flux density is proportional to the current (I) times the number of turns(N), hence F=I*N, called the magnetomotive force (F). One way to reduce the winding losses, but still give a high magnetic flux density is to, keep in mind the P=I^2*R equation, increase the number of turns and reduce the current, keeping F constant. Thus, decreasing I but increasing R due to the increased length/number of turns. Observing that I is squared, follows that the power losses decreases.

Other losses associated are the core losses. These are related to the ferromagnetic material making the core (magnetic path of the electromagnet), if the magnet has a core.
https://en.wikipedia.org/wiki/Magnetic_core#Core_loss
The core losses are separated by the magnetic domain movement and eddy currents (induced currents) in the core. The magnetic domain movement are proportional to the changing magnetic flux density squared times the amplitude of the flux density.

Eddy currents are a consequence of a changing magnetic flux density in a conductive material. And the associated losses are proportional to the current density squared and the conductivity.

The above losses is mostly occurring using AC (alternating current) for the winding excitation, or if the material is moving in a magnetic field. Or if the external field is alternating.

An electromagnet can have both AC and DC winding excitation, that is application specific. In your case, the option is to use permanent magnets, so I would conclude that the electromagnet is powered by DC. But using DC excitation, the core losses is minimal if no movement or external field is applied. So in that case, I would say that the winding losses are the most pronounced source of heat.
 

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