Radiated energy by decelerating (relativistic) point charge

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SUMMARY

The discussion focuses on calculating the total radiated energy by a relativistically moving point charge subjected to a constant decelerating force. The relevant equations include Lienard's equation for total radiated power and the modified Newton's law of motion incorporating radiation reaction. The user attempts to derive the acceleration and velocity over time, ultimately considering a conservation of energy approach to simplify the calculation. The conclusion suggests that the radiated energy can be expressed as the difference between the initial kinetic energy and the work done against the applied force.

PREREQUISITES
  • Understanding of Lienard's equation for radiated power
  • Familiarity with relativistic mechanics and the concept of Lorentz factor
  • Knowledge of conservation of energy principles in physics
  • Ability to solve differential equations related to motion
NEXT STEPS
  • Study the derivation and implications of Lienard's equation in detail
  • Learn about the Abraham-Lorentz force and its role in radiation reaction
  • Explore advanced topics in relativistic dynamics and energy conservation
  • Practice solving differential equations in the context of relativistic motion
USEFUL FOR

Physics students, researchers in electromagnetism, and anyone interested in the dynamics of charged particles under relativistic conditions.

taha.hojati
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Homework Statement


A point charge q is moving relativistically with constant speed ##\beta## along the x-axis.
At t = 0 a constant decelerating force F is applied in opposite direction of
its velocity. If the charge stops after traveling a distance d, find the total radiated
energy.


Homework Equations


I found these equations in Griffith's book:

Total radiated power by a relativistically moving point charge (Lienard's eq.):
$$P = \frac{\mu_0 q^2 \gamma^6}{6 \pi c} (a^2 - |\frac{\beta \times a }{c} | ) $$ Here again ##\beta## is the the velocity of the charge (in SI units), and a is its acceleration.

Newton's law of motion for charged particle (with radiation reaction):
$$a= \tau \dot{a} + \frac{F}{m}$$ here ##\tau = \frac{\mu_0 q^2}{6 \pi c } ##, (## m \tau \dot{a} ## is the abraham-lorentz formula for the radiation reaction).
This equation is from Griffith's book but I am a little confused by it because in relativity we have ##F_{net} = \frac{d}{dt} \gamma m v \neq m a##.

The Attempt at a Solution



First I tried to find acceleration and velocity based on time by solving the differential equation ==>
$$ a = -\frac{F}{m} e^{t/\tau} + \frac{F}{m} $$
$$\Rightarrow v= \beta + \frac{F}{m} ( t - e^{t/\tau})$$
From here I wanted to find ##t_{final}## based on d and then calculate the total energy radiated by integrating the Lienard's equation, but I am unsure since it seems like I am forgetting all I learned about relativity in my mechanics class (also the integral is hard).

So I thought I can approach from conservation of energy aspect. So total kinetic energy is ##KE_{initial} = (\gamma-1) m c^2 ##. Now part of this energy is radiated and the rest is spent on resisting the force F. So can I just write ##E_{rad} = KE_{initial} - F d ## ? That would make everything easier. Thanks in advance!
 
Physics news on Phys.org
You know that before the force is applied there is no radiation. You also know that the acceleration is in the opposite direction of the velocity. The cross product of any two col-linear vectors is 0 so you can drop the cross product term.
 

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