What Happens When You Misapply the Lorentz Force Equation?

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SUMMARY

The discussion focuses on the misapplication of the Lorentz Force equation in the context of a particle moving in a constant magnetic field. The correct formulation of the equations of motion is given by the vector equation \(m \frac{\mathrm{d} \vec{v}}{\mathrm{d}t} = q \vec{v} \times \vec{B}\), where \(\vec{B} = B \vec{e}_z\). The integration of these equations leads to a clear understanding of the motion in three dimensions, particularly emphasizing the simplicity of solving for \(v_z\) and the method to derive \(v_x\) and \(v_y\) through elimination techniques. The discussion highlights the importance of maintaining vector notation rather than reducing it to scalar equations.

PREREQUISITES
  • Understanding of the Lorentz Force Law
  • Familiarity with vector calculus
  • Knowledge of classical mechanics, specifically motion in magnetic fields
  • Basic proficiency in solving differential equations
NEXT STEPS
  • Study the derivation of the Lorentz Force equation in detail
  • Learn about the motion of charged particles in magnetic fields
  • Explore vector calculus applications in physics
  • Investigate numerical methods for solving differential equations in mechanics
USEFUL FOR

Physics students, educators, and professionals in fields related to electromagnetism and classical mechanics will benefit from this discussion, particularly those interested in the dynamics of charged particles in magnetic fields.

Gabriele Pinna
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We know that Lorentz Force is a centripetal force so:
$$qVBsenx=m\frac{v^2}{r}$$ and the value of V is constant (but not the direction)
But if we write:
$$qvBsenx=m\frac{dV}{dt}$$
we obtain that v is exponential.
What is wrong ?
 
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I guess you want to solve the nonrelativistic equation of motion for a particle in a constant magnetic field. Let's put ##\vec{B}=B \vec{e}_z##. Then the equations of motion read (in SI units)
$$m \frac{\mathrm{d} \vec{v}}{\mathrm{d}t} = q \vec{v} \times \vec{B}.$$
In components you have
$$\begin{pmatrix} \dot{v}_x \\ \dot{v}_y \\ \dot{v}_z \end{pmatrix}=\frac{qB}{m} \begin{pmatrix} v_y \\ -v_x \\ 0 \end{pmatrix}=\omega \begin{pmatrix} v_y \\ -v_x \\ 0\end{pmatrix}.$$
Now you can integrate the equations of motion quite easily. I give some hints:

The equation for ##v_z## is very simple. This you should be able to solve very easily.

To solve also for ##v_x## and ##v_y##, just take the time derivative of the equation for ##v_x## and use the 2nd equation to eliminate ##v_y##. Then you have a equation for ##v_x## alone, which is quite easy to solve too.

Once you have ##\vec{v}## just take one more integration to get ##\vec{x}##.
 
You are trying to write a vector equation as a single scalar equation.
 

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