Runge-kutta method for a force acting upon a charged particle

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SUMMARY

The discussion focuses on implementing the Runge-Kutta method to model the movement of a charged particle in an electric field using Fortran 90. The Lorentz force equation, F=q(E+vxB), is utilized to derive the ordinary differential equations (ODEs) necessary for the simulation. The key equations derived are dv/dt = F(x,v)/m and dx/dt = v, which are essential for applying the Runge-Kutta method to plot the position versus time graph of the test charge.

PREREQUISITES
  • Understanding of ordinary differential equations (ODEs)
  • Familiarity with the Lorentz force equation
  • Knowledge of Fortran 90 programming
  • Basic concepts of kinematics, specifically acceleration and velocity
NEXT STEPS
  • Study the implementation of the Runge-Kutta method in Fortran 90
  • Learn how to derive and solve ordinary differential equations
  • Explore the physics of electric fields and forces on charged particles
  • Research numerical methods for solving differential equations
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Students in physics or engineering, programmers working with numerical simulations, and anyone interested in modeling charged particle dynamics in electric fields.

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I have this project that involves the runge-kutta method, and I honestly have no clue what I am doing.

I never learned about this before, and I don't know much about ordinary differential equations. I am learning all of this next semester but it is required information for this project.

In my project, I have to model the movement of a test charge through an electric field and program it onto fortran 90.

I know that the Lorentz equation is F=q(E+vxB), and also F=ma (as a special case), and I can equate the two to find acceleration.

I have no idea how I would set this up as an ODE and then use the runge-kutta method. I need to do this so that I can plot a position vs. time graph of the test charge.

Can someone please help me out?
 
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Acceleration is the second derivative of position (x) with respect to time.
The first derivative is velocity (v). It follows that acceleration is the derivative of velocity.

Thus, as a first order ODE, F = ma becomes
<br /> \frac {dv}{dt} = F(x,v)/m = (q/m)(E + v \times B) \\<br /> \frac{dx}{dt} = v<br />

At this point you can use Runge-Kutta.
 

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