Lorentz Force Equation – Is vxB Representable?

AI Thread Summary
The discussion centers on the Lorentz force equation, F = qE + qvxB, and whether the term vxB can be represented as a gradient of a meaningful quantity. It is noted that while electric fields can be expressed as the gradient of electric potential, the magnetic force, represented by vxB, does not fit this model since it is not conservative. Participants express confusion over differing opinions on whether magnetic fields can be considered conservative forces, with references to external sources that support both views. Ultimately, the consensus is that the magnetic force depends on velocity, complicating the potential energy formulation. The conversation highlights the complexities of relating magnetic forces to potential energy in physics.
Michael Lin
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Hi All,

Just a thought. The Lorentz force equation as we all know is: F = qE + qvxB. We know that Electrical Field can be written as del(Phi), where Phi is the electrical potential. Also, Force can be written as del(Energy) - correct me on this one. Hence is there a representative term for vxB. Can vxB be written as del(something) where something is a meaningful quantity?

Just curious,
Thanks - Michael
 
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It sure can. Taking \vec{F}=-\vec{\nabla}U and \vec{E}=-\vec{\nabla}\Phi, we have:

-\vec{\nabla}U=-q\vec{\nabla}\Phi+q\vec{v}\times\vec{B}.

Rearranging terms we get:

q\vec{v}\times\vec{B}=q\vec{\nabla}\Phi-\vec{\nabla}U.

Thanks to the linearity of the \vec{\nabla} operator, we have:

q\vec{v}\times\vec{B}=\vec{\nabla}(q\Phi-U)
\vec{v}\times\vec{B}=\vec{\nabla}(\Phi-\frac{U}{q}).
 
But a U that satisfies \vec{F}=-\vec{\nabla}U exists only if \vec F is a conservative force. The magnetic force isn't conservative.
 
Duh. :frown:

Well boys and girls, this is what happens when plug-n-chug runs amuck.

Is it 5:00 yet?
 
If a force is conservative, you can define a potential energy function for it. The potential energy of a particle can depend only on its position, so a conservative force can depend only on position. But the magnetic force on a particle depends on the velocity (both magnitude and direction!) of the particle, not just on its position (which determines the magnetic field).
 
how can we get potential from lorentz equations...?
 
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