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Question: In the x-y plane, the region \[y > 0\] has a uniform magnetic field \[{B_1}\widehat {\text{k}}\] and...

In the x-y plane, the region y>0y > 0 has a uniform magnetic field B1k^{B_1}\widehat {\text{k}} and the region y<0y < 0 has another uniform magnetic field B2k^{B_2}\widehat {\text{k}}. A positively charged particle is projected from the origin along the positive y-axis with speed Vo=πms - 1{V_o} = \pi \,{\text{m}}{{\text{s}}^{{\text{ - 1}}}} at t=0t = 0, as shown in the figure. Neglect gravity in this problem. Let t=Tt = T be the time when the particle crosses the x-axis from below for the first time. If B2=4B1{B_2} = 4{B_1}, the average speed of the particle, in ms - 1{\text{m}}{{\text{s}}^{{\text{ - 1}}}}, along the x-axis in the time interval TT is _________.

Explanation

Solution

We are asked to find the average speed. For this we need to check the path that the charged particle will follow in a uniform magnetic field. Find the total distance travelled by the particle and the total time taken. Using these two values find the average speed of the particle.

Complete step by step solution:
Given, for the region y>0y > 0, the magnetic field is B1k^{B_1}\widehat {\text{k}}
For the region y<0y < 0, the magnetic field is B2k^{B_2}\widehat {\text{k}}
The velocity of the charged particle is Vo=πms - 1{V_o} = \pi \,{\text{m}}{{\text{s}}^{{\text{ - 1}}}} at t=0t = 0.
The particle crosses the x-axis at t=Tt = T
And B2=4B1{B_2} = 4{B_1}.
The particle is said to be positively charged, let the charge of the particle be qq
Let the mass of the charged particle be mm
Here, the particle starts from origin and moves towards the positive y-axis also, a uniform magnetic field exists along the z-axis. When a charged particle motion is kept in a uniform magnetic field and direction of motion of the particle is perpendicular to the direction of magnetic field, then the charged particle experiences a force due to which the charged particle follows a curved path. The radius of this curved path is given by,
r=mvqBr = \dfrac{{mv}}{{qB}} ……………..(i)

where mm is the mass of the charged particle, vv is the velocity of the charged particle, BB is the magnetic field strength and qq is the charge of the particle.
The time period of this circular motion is given by,
T=2πmqBT = \dfrac{{2\pi m}}{{qB}} ………………...(ii)
Since here, the motion of the charged particle is perpendicular to the direction of magnetic field, so the charged particles will follow a circular path in both y>0y > 0 region and y<0y < 0 region.
Let RR be the radius of the circular path for region y>0y > 0 and rr be the radius of the circular path for region y<0y < 0.
Let us draw a diagram for proper understanding.

The radius rr is less than RR, as from equation (i), we observe the larger the magnetic field, the smaller is the radius.
Now, using the formula from equation (i), we get the radius RR for region y>0y > 0.
R=mV0qB1R = \dfrac{{m{V_0}}}{{q{B_1}}} ………………...(iii)
The radius rr for region y<0y < 0, using the formula from equation (i) is
r=mV0qB2r = \dfrac{{m{V_0}}}{{q{B_2}}} ……………….(iv)
We have B2=4B1{B_2} = 4{B_1}, substituting this value in equation (iv) we get
r=mV04qB1r = \dfrac{{m{V_0}}}{{4q{B_1}}} ……………….(v)
Now, from the figure, we observe that the total distance travelled by the particle is
S=2R+2rS = 2R + 2r
Putting the values from equations (iii) and (v) in the above equation we get
S=2(mV0qB1)+2(mV04qB1)S = 2\left( {\dfrac{{m{V_0}}}{{q{B_1}}}} \right) + 2\left( {\dfrac{{m{V_0}}}{{4q{B_1}}}} \right)
S=2mV0qB1+mV02qB1\Rightarrow S = \dfrac{{2m{V_0}}}{{q{B_1}}} + \dfrac{{m{V_0}}}{{2q{B_1}}}
S=5mV02qB1\Rightarrow S = \dfrac{{5m{V_0}}}{{2q{B_1}}}
Now, the total time taken by the particle is addition of the time taken to complete the upper half circle and time taken to complete the lower half circle.
That is,
T=T1+T2T = {T_1} + {T_2} ……………...(vi)
where T1{T_1} is the time period for the upper half circle and T2{T_2} is the time period for the lower half circle.
We can write, from equation (ii)
T1=12×2πmqB1{T_1} = \dfrac{1}{2} \times \dfrac{{2\pi m}}{{q{B_1}}} (half becomes its for half circle)
Similarly,
T2=12×2πmqB2{T_2} = \dfrac{1}{2} \times \dfrac{{2\pi m}}{{q{B_2}}}
Putting these values in equation (vi) and substituting B2=4B1{B_2} = 4{B_1}, we get
T=12×2πmqB1+12×2πm4qB1T = \dfrac{1}{2} \times \dfrac{{2\pi m}}{{q{B_1}}} + \dfrac{1}{2} \times \dfrac{{2\pi m}}{{4q{B_1}}}
T=πmqB1+πm4qB1\Rightarrow T = \dfrac{{\pi m}}{{q{B_1}}} + \dfrac{{\pi m}}{{4q{B_1}}}
T=5πm4qB1\Rightarrow T = \dfrac{{5\pi m}}{{4q{B_1}}}
Now, average speed of the particle will be,
Vav=Total distance travelledtotal time{V_{av}} = \dfrac{{{\text{Total distance travelled}}}}{{{\text{total time}}}}
Here,
Vav=ST{V_{av}} = \dfrac{S}{T}
Putting the values of SS and TT, we get

\right)}}$$ $${V_{av}} = 2\,{\text{m}}{{\text{s}}^{{\text{ - 1}}}}$$ **Therefore, the average speed is $$2\,{\text{m}}{{\text{s}}^{{\text{ - 1}}}}$$.** **Note:** Always keep in mind that a charged particle in a uniform magnetic field will follow a curved path only when the motion of the particle and direction of magnetic field are perpendicular to each other, if they are parallel then the charged particle will not experience any magnetic force.