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netineya [11]
3 years ago
12

A charge is accelerated from rest through a potential difference V and then enters a uniform magnetic field oriented perpendicul

ar to its path. The magnetic field deflects the particle into a circular arc of radius R. If the accelerating potential is tripled to 3V, the radius of the circular arc will now be:
Physics
1 answer:
vodomira [7]3 years ago
6 0

Answer:

New radius of the charge particle when potential is increased by 3times of initial value

R' = \sqrt3 R

Explanation:

As we know that charge particle is accelerated due to potential difference V then we have

\frac{1}{2}mv^2 = qV

now the speed of the charge particle is given as

v = \sqrt{\frac{2qV}{m}}

now in constant magnetic field which is perpendicular to the motion of charge  we have

qvB = \frac{mv^2}{R}

now we have

R = \frac{mv}{qB}

now we have

R = \frac{m}{qB} \times \sqrt{\frac{2qV}{m}}[/tex]

R = \frac{1}{B} \sqrt{\frac{2mV}{q}}

now if we changed the potential to three times of initial value then we have

R' = \frac{1}{B} \sqrt{\frac{2m(3V)}{q}}

so we have

\frac{R}{R'} = \frac{1}{\sqrt3}

R' = \sqrt3 R

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Answer:

R \approx 2.418\times 10^{9}\,km

Explanation:

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Supóngase que el planeta tiene una órbita circular, el período de rotación del planeta es:

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Asimismo, la rapidez angular se describe como función de la aceleración centrípeta:

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Ahora se reemplaza en la ecuación de período:

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La distancia del planeta con respecto al sol es finalmente despejada:

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Finalmente, se sustituyen las variables y se determina la distancia:

R = \sqrt[3]{\left(6.674\times 10^{-11}\,\frac{N\cdot m^{2}}{kg^{2}} \right)\cdot (1.989\times 10^{30}\,kg)\cdot \left[\frac{(65\,a)\cdot \left(365\,\frac{d}{a} \right)\cdot \left(86400\,\frac{s}{d} \right)}{2\pi} \right]^{2}}

R \approx 2.418\times 10^{12}\,m

R \approx 2.418\times 10^{9}\,km

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