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Question: A beam of a mixture of \( \alpha \) particles and protons are accelerated through the same potential...

A beam of a mixture of α\alpha particles and protons are accelerated through the same potential difference before entering into the magnetic field of strength BB . If r1=5cm{r_1} = 5cm , then r2{r_2} is

(A) 5  cm5\;cm
(B) 52cm5\sqrt 2 cm
(C) 102cm10\sqrt 2 cm
(D) 20  cm20\;cm

Explanation

Solution

We know that both alpha particles and protons are charged particles. If a charged particle perpendicular to the uniform magnetic field. The magnetic Lorentz force is acting perpendicular to the velocity. This supplies the necessary centripetal force required for circular motion.

Formula used:
v=qBrmv = \dfrac{{qBr}}{m}
Where vv is the velocity of the particle, qq stands for the charge of the particle, BB stands for the magnetic field, rr is the radius of the circular path, and mm is the mass of the particle.

Complete Step by step solution:
The velocity of a charged particle moving in a circular path in a uniform magnetic field is given by,
v=qBrmv = \dfrac{{qBr}}{m}
From this equation, we can write the expression for radius as,
r=mvqBr = \dfrac{{mv}}{{qB}}
We know that the momentum of the particle,
P=mvP = mv
Therefore, the radius can be written as
r=PqBr = \dfrac{P}{{qB}}
We know that momentum can be written as,
P=2mEP = \sqrt {2mE}
Substituting in the above equation, we get
r=2mEqBr = \dfrac{{\sqrt {2mE} }}{{qB}}
We can write the energy of a charged particle in a potential VV as,
E=qVE = qV
Substituting in the above equation, we get
r=2mqVqBr = \dfrac{{\sqrt {2mqV} }}{{qB}}
This equation can be rearranged as,
r=mq2VBr = \sqrt {\dfrac{m}{q}} \dfrac{{\sqrt {2V} }}{B}
The radius r1{r_1} can be written as,
r1=m1q12VB{r_1} = \sqrt {\dfrac{{{m_1}}}{{{q_1}}}} \dfrac{{\sqrt {2V} }}{B}
The radius r2{r_2} can be written as,
r2=m2q22VB{r_2} = \sqrt {\dfrac{{{m_2}}}{{{q_2}}}} \dfrac{{\sqrt {2V} }}{B}
The ratio of the two radii can be written as,
r2r1=m2q22VBm1q12VB\dfrac{{{r_2}}}{{{r_1}}} = \dfrac{{\sqrt {\dfrac{{{m_2}}}{{{q_2}}}} \dfrac{{\sqrt {2V} }}{B}}}{{\sqrt {\dfrac{{{m_1}}}{{{q_1}}}} \dfrac{{\sqrt {2V} }}{B}}}
Cancelling the common terms and rearranging, we get
r2r1=m2q2×q1m1\dfrac{{{r_2}}}{{{r_1}}} = \sqrt {\dfrac{{{m_2}}}{{{q_2}}}} \times \sqrt {\dfrac{{{q_1}}}{{{m_1}}}}
This can be written as,
r2r1=m2m1×q1q2\dfrac{{{r_2}}}{{{r_1}}} = \sqrt {\dfrac{{{m_2}}}{{{m_1}}}} \times \sqrt {\dfrac{{{q_1}}}{{{q_2}}}}
We know that the mass of an alpha particle is four times that of the mass of protons. i.e.
mα=4mp{m_\alpha } = 4{m_p}
Here m2{m_2} is the mass of the alpha particle and mp{m_p} is the mass of the proton.
Therefore we can write,
m2m1=41\sqrt {\dfrac{{{m_2}}}{{{m_1}}}} = \sqrt {\dfrac{4}{1}}
Also, the charge of alpha particles are two times that of the charge of protons, i.e.
qα=2qp{q_\alpha } = 2{q_p}
Here q2{q_2} is the charge of the alpha particle and q1{q_1} is the charge of the proton, then we can write
q2=2qp{q_2} = 2{q_p}
Then the ratio will be
q1q2=12\sqrt {\dfrac{{{q_1}}}{{{q_2}}}} = \sqrt {\dfrac{1}{2}}
Putting these values in the expression
r2r1=m2m1×q1q2\dfrac{{{r_2}}}{{{r_1}}} = \sqrt {\dfrac{{{m_2}}}{{{m_1}}}} \times \sqrt {\dfrac{{{q_1}}}{{{q_2}}}}
We get,
r2r1=41×12=2\dfrac{{{r_2}}}{{{r_1}}} = \sqrt {\dfrac{4}{1}} \times \sqrt {\dfrac{1}{2}} = \sqrt 2
From this r2=r12{r_2} = {r_1}\sqrt 2
It is given that, the value of r1=5cm{r_1} = 5cm
Then,
r2=52cm{r_2} = 5\sqrt 2 cm
The answer is: Option (B): 52cm5\sqrt 2 cm .

Note:
The radius r=mvqBr = \dfrac{{mv}}{{qB}} is known as the cyclotron radius. A cyclotron is a device employed to accelerate charged particles to high energies. It works on the principle that a charged particle moving normal to magnetic flux experiences magnetic Lorentz force. Because of this force, the particle moves in a circular path.