- #1
andresordonez
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SOLVED
(Problem 10, Chapter 2, Modern Physics - Serway)
Recall that the magnetic force on a charge q moving with velocity [tex]\vec{v}[/tex] in a magnetic field [tex]\vec{B}[/tex] is equal to [tex]q\vec{v}\times\vec{B}[/tex]. If a charged particle moves in a circular orbit with a fixed speed [tex]v[/tex] in the presence of a constant magnetic field, use the relativistic form of Newton's second law to show that the frequency of its orbital motion is
[tex]
f=\frac{qB}{2\pi m}(1-\frac{v^2}{c^2})^{1/2}
[/tex]
[tex]
F=\frac{ma}{(1-v^2/c^2)^{3/2}}
[/tex]
The particle moves in a circle then the magnetic field is perpendicular to the velocity and [tex]F=qvB[/tex].
[tex]
f=\frac{v}{2\pi R}
[/tex]
[tex]
qvB=\frac{ma}{(1-v^2/c^2)^{3/2}}
=\frac{m}{(1-v^2/c^2)^{3/2}}\frac{v^2}{R}
[/tex]
[tex]
R=\frac{mv}{(1-v^2/c^2)^{3/2}qB}
[/tex]
[tex]
f=\frac{(1-v^2/c^2)^{3/2}qB}{2\pi m}
[/tex]
What's wrong?
(Problem 10, Chapter 2, Modern Physics - Serway)
Homework Statement
Recall that the magnetic force on a charge q moving with velocity [tex]\vec{v}[/tex] in a magnetic field [tex]\vec{B}[/tex] is equal to [tex]q\vec{v}\times\vec{B}[/tex]. If a charged particle moves in a circular orbit with a fixed speed [tex]v[/tex] in the presence of a constant magnetic field, use the relativistic form of Newton's second law to show that the frequency of its orbital motion is
[tex]
f=\frac{qB}{2\pi m}(1-\frac{v^2}{c^2})^{1/2}
[/tex]
Homework Equations
[tex]
F=\frac{ma}{(1-v^2/c^2)^{3/2}}
[/tex]
The Attempt at a Solution
The particle moves in a circle then the magnetic field is perpendicular to the velocity and [tex]F=qvB[/tex].
[tex]
f=\frac{v}{2\pi R}
[/tex]
[tex]
qvB=\frac{ma}{(1-v^2/c^2)^{3/2}}
=\frac{m}{(1-v^2/c^2)^{3/2}}\frac{v^2}{R}
[/tex]
[tex]
R=\frac{mv}{(1-v^2/c^2)^{3/2}qB}
[/tex]
[tex]
f=\frac{(1-v^2/c^2)^{3/2}qB}{2\pi m}
[/tex]
What's wrong?
Last edited: