Lorentz Force in conductive beam

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SUMMARY

The Lorentz force acting on a rectangular beam carrying current in a magnetic field is expressed as a distributed load across the beam. The force can be calculated using the integral of the current density (J) over the beam's cross-section, rather than using total current (I). For low-frequency or direct current applications, the current density may be approximated as constant, but this depends on material properties and voltage application. Understanding these factors is crucial for accurately modeling the force distribution along the beam.

PREREQUISITES
  • Understanding of Lorentz force principles
  • Knowledge of current density (J) and its calculation
  • Familiarity with integral calculus in physics
  • Basic concepts of electromagnetic fields
NEXT STEPS
  • Research the calculation of current density in conductive materials
  • Study the application of integrals in force distribution analysis
  • Explore the effects of material properties on current flow in beams
  • Learn about the implications of low-frequency versus high-frequency currents on force distribution
USEFUL FOR

Physicists, electrical engineers, and students studying electromagnetism and material science will benefit from this discussion, particularly those interested in the behavior of conductive beams in magnetic fields.

diemilio
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It is known that in a current carrying wire, exposed to a magnetic field, the wire will experience a force equal to the product of the field, the current and the length of the wire (where the direction of the force is orthogonal to both the field and the direction along the length of the beam). F = B*I*L

Now, in a rectangular beam of length L, width w, and height h (where w<<h<<L), again carrying a current and in the presence of a magnetic field, how is the Lorentz force expressed? is the force acting as a distributed load all along the beam? is this integrated force modeled as a point load at the center of the beam? Is it acting as a body load? a surface load? Could someone help me understand this??

Thanks in advance,

diemilio
 
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diemilio said:
It is known that in a current carrying wire, exposed to a magnetic field, the wire will experience a force equal to the product of the field, the current and the length of the wire (where the direction of the force is orthogonal to both the field and the direction along the length of the beam). F = B*I*L

Now, in a rectangular beam of length L, width w, and height h (where w<<h<<L), again carrying a current and in the presence of a magnetic field, how is the Lorentz force expressed? is the force acting as a distributed load all along the beam? is this integrated force modeled as a point load at the center of the beam? Is it acting as a body load? a surface load? Could someone help me understand this??

Thanks in advance,

diemilio

In such a case the force is distributed, and it would be important to know the current density (current per unit area) in the beam. For a low frequency, or direct current, you may be able to approximate the current density distribution as constant across the beam, but it really depends on the material properties and how the voltage is applied to the ends of the beam.

In general the force would be expressed as an integral over the volume of the beam. The Lorenz force is really force per unit length, and the surface integral is taken over the cross section in terms of current density J, rather than current I.
 
Nice! Got it! Thank you so much for the quick reply!

diemilio
 

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