The Lorentz force causes charged particles to orbit around magnetic field lines.  At what rate do protons orbit around a field line?  Assume the protons have energy of 1 MeV and are in a magnetic field with strength B = 2.4×10-7 T.  Find the orbital frequency in revolutions/second (Hz); express answer to 3 significant digits. The protons orbit the field at  _____ Hz.

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Chapter9: Relativity
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The Lorentz force causes charged particles to orbit around magnetic field lines.  At what rate do protons orbit around a field line?  Assume the protons have energy of 1 MeV and are in a magnetic field with strength B = 2.4×10-7 T.  Find the orbital frequency in revolutions/second (Hz); express answer to 3 significant digits.

The protons orbit the field at  _____ Hz.

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How would the answer to the previous problem change if the particles were 1 MeV electrons, instead of protons?

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The Lorentz force that makes a charged particle move in a circular path in a magnetic field is given by

F=qvBF=qvB

where qq is the charge of the particle, vv is the speed of the particle, and BB is the magnetic field strength.

Since the particle is moving in a circular path, this force must equal the centripetal force, F=mv2rF=rmv2​, where mm is the mass of the particle and rr is the radius of the circular path.

Setting the two expressions for FF equal to each other, we get

qvB=mv2rqvB=rmv2​

Since we want to find the frequency of the orbit, we need to find the speed vv of the proton. Given that the energy of the proton is 1 MeV, we can write

12mv2=1 MeV21​mv2=1MeV

and solve for vv:

v=2×1 MeVmv=m2×1MeV​​

where mm is the mass of a proton, which is approximately 1.67×10−27 kg1.67×10−27kg.

Substituting this expression for vv into the expression for the Lorentz force, we can solve for the frequency of the orbit. The frequency is related to the speed and the radius of the path by

f=v2πrf=2πrv​

Substituting our expressions for vv and rr, we find

f=qB2πmf=2πmqB​

Substituting the given values for the charge of a proton (q=1.6×10−19 Cq=1.6×10−19C), the magnetic field strength (B=2.4×10−7 TB=2.4×10−7T), and the mass of a proton, we get

f≈(1.6×10−19 C)(2.4×10−7 T)2π(1.67×10−27 kg)≈(1.6)(2.4×10−7)2π(1.67×10−27)×106 eVf≈2π(1.67×10−27kg)(1.6×10−19C)(2.4×10−7T)​≈2π(1.67×10−27)(1.6)(2.4×10−7)​×106eV

f≈3.84×10−73.14×1.67×10−27×106 eVf≈3.14×1.67×10−273.84×10−7​×106eV

f≈3.843.14×1.67×1014 Hzf≈3.14×1.673.84​×1014Hz

f≈3.845.24×1014 Hzf≈5.243.84​×1014Hz

f≈0.733×1014 Hzf≈0.733×1014Hz

f≈73.3×1012 Hzf≈73.3×1012Hz

So the protons orbit the field at 73.3×1012 Hz73.3×1012Hz, or 73.3 THz73.3THz.

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