Electromagnetic radiation is emitted by accelerating charges. The rate at which energy is emitted from an accelerating charge that has charge q and acceleration a is given by dEdt=q2a26πϵ0c3 where c is the speed of light. If a proton with a kinetic energy of 5.0 MeV is traveling in a particle accelerator in a circular orbit with a radius of 0.530 m, what fraction of its energy does it radiate per second?

Respuesta :

Given Information:

Kinetic energy of proton = KE = 5 MeV

Radius = R = 0530 m

Speed of light = c = 3x10⁸ m/s

Permittivity of free space = ε = 8.854×10⁻¹² F/m

Mass of proton m = 1.67x10⁻²⁷ kg

Required Information:

Energy radiated per second = dE/dt = ?

Answer:

[tex]\frac{dE}{dt} = 7.346x10^{14}[/tex] [tex]eV/s[/tex]

Explanation:

The rate at which energy is emitted from an accelerating charge with charge q and acceleration a is given by

[tex]\frac{dE}{dt} =\frac{q^{2}a^{2} }{6\pi{\epsilon}c^{3}}[/tex]  

Where ε is the permittivity of free space and c is the speed of light

We know that centripetal acceleration is given by

[tex]a = \frac{v^2}{R}[/tex]

Whereas kinetic energy is given by

[tex]KE = \frac{1}{2}mv^{2}[/tex]

[tex]\frac{2KE}{m} = v^2[/tex]

Substitute in the equation of acceleration

[tex]a = \frac{2KE}{mR}[/tex]

[tex]a=1.13x10^{34}[/tex] [tex]eV/s^{2}[/tex]

Therefore, the corresponding energy radiated per second is

[tex]\frac{dE}{dt} =\frac{(1.60x10^{-19})^{2}(1.13x10^{34})^{2} }{6\pi{\epsilon}c^{3}}[/tex]

[tex]\frac{dE}{dt} =\frac{3.27x10^{30} }{6\pi8.854x10^{-12}(3x10^{8}^)^{3}}[/tex]

[tex]\frac{dE}{dt} = 7.346x10^{14}[/tex] [tex]eV/s[/tex]

The energy radiated by the proton is 7.346×10¹⁴ eV/s.

Electromagnetic radiation:

The rate at which energy is emitted from an accelerating charge that has charge q and acceleration a is given by:

[tex]\frac{dE}{dt}=\frac{q^2a^2}{6\pi\epsilon_oc^3}[/tex]

where q is the charge of the particle, and

a is the acceleration

It is given that a proton with kinetic energy (KE) of 5.0 MeV is traveling in a particle accelerator in a circular orbit with a radius (r) of 0.530 m

The acceleration of the particle in the circular orbit is given by:

[tex]a=\frac{v^2}{r}[/tex]

The kinetic energy is given by:

[tex]KE=\frac{1}{2}mv^2[/tex]

where m = 1.67×10⁻²⁷ kg is the mass of the proton

so,

[tex]5\times10^6\;eV=\frac{1}{2}\times1.67\times10^{-27}kg\times v^2\\\\v^2\approx6\times10^{33}eV/kg[/tex]

so acceleration:

[tex]a=\frac{v^2}{r}=\frac{6\times10^{33}}{0.53} \\\\a=1.13\times10^{34}\;eV/kgm[/tex]

now, we can calculate the energy radiated:

[tex]\frac{dE}{dt}=\frac{q^2a^2}{6\pi\epsilon_oc^3}=\frac{1.6\times10^{-19}\times(1.13\times10^{34})^2}{6\pi\times8.85\times10^{-12}\times(3\times10^8)^3}\\\\\frac{dE}{dt}=7.346\times10^{14}\;eV/s[/tex]

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