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Question: The arrangement shown is placed in a vertical uniform magnetic field. The rods are of same length /a...

The arrangement shown is placed in a vertical uniform magnetic field. The rods are of same length /and masses m. Initially they are placed in contact parallel to each other and pulled apart from rest such that net force (due to external as well as due to magnetic interaction) on rod at any instant is F. The current through resistor at an instant when rods are at separation 2s is BlRαFSm\frac{Bl}{R}\sqrt{\frac{\alpha FS}{m}}. Find α\alpha

Answer

8

Explanation

Solution

The problem describes a system where two parallel conducting rods of length ll and mass mm are placed on conducting rails in a uniform magnetic field BB. A resistor RR connects the rails. The rods are pulled apart from rest such that the net force on each rod at any instant is FF. We need to find the value of α\alpha in the given expression for the current I=BlRαFSmI = \frac{Bl}{R}\sqrt{\frac{\alpha FS}{m}} when the separation between the rods is 2S2S.

  1. Net Force and Acceleration: The problem states that the net force on each rod at any instant is FF. Since the mass of each rod is mm, the acceleration of each rod is constant: a=Fma = \frac{F}{m}

  2. Kinematics of the Rods: Let the rods start from rest at t=0t=0 when their separation is zero. Due to the constant net force FF on each rod, they will accelerate away from each other. Let x1x_1 be the distance moved by the left rod and x2x_2 be the distance moved by the right rod. Since their accelerations are equal (a=F/ma = F/m) and they start from rest, their velocities and displacements will be equal at any time tt: v1=v2=at=(Fm)tv_1 = v_2 = at = \left(\frac{F}{m}\right)t x1=x2=12at2=12(Fm)t2x_1 = x_2 = \frac{1}{2}at^2 = \frac{1}{2}\left(\frac{F}{m}\right)t^2

  3. Total Separation and Relative Velocity: The total separation between the rods at time tt is x=x1+x2x = x_1 + x_2. x=12(Fm)t2+12(Fm)t2=(Fm)t2x = \frac{1}{2}\left(\frac{F}{m}\right)t^2 + \frac{1}{2}\left(\frac{F}{m}\right)t^2 = \left(\frac{F}{m}\right)t^2 The relative velocity (speed at which the separation increases) is vrel=v1+v2v_{rel} = v_1 + v_2. vrel=(Fm)t+(Fm)t=2(Fm)tv_{rel} = \left(\frac{F}{m}\right)t + \left(\frac{F}{m}\right)t = 2\left(\frac{F}{m}\right)t

  4. Time to reach separation 2S2S: We are interested in the instant when the separation is 2S2S. Using the expression for total separation: 2S=(Fm)t22S = \left(\frac{F}{m}\right)t^2 Solving for t2t^2: t2=2SmFt^2 = \frac{2Sm}{F} So, t=2SmFt = \sqrt{\frac{2Sm}{F}}

  5. Relative Velocity at separation 2S2S: Substitute the value of tt into the expression for vrelv_{rel}: vrel=2(Fm)2SmFv_{rel} = 2\left(\frac{F}{m}\right)\sqrt{\frac{2Sm}{F}} To simplify, bring the 2(F/m)2(F/m) inside the square root: vrel=(2Fm)22SmF=4F2m22SmF=8F2Smm2F=8FSmv_{rel} = \sqrt{\left(2\frac{F}{m}\right)^2 \frac{2Sm}{F}} = \sqrt{4\frac{F^2}{m^2} \frac{2Sm}{F}} = \sqrt{\frac{8F^2Sm}{m^2F}} = \sqrt{\frac{8FS}{m}}

  6. Induced EMF and Current: The induced electromotive force (EMF) in the circuit due to the relative motion of the rods is given by: E=Blvrel\mathcal{E} = B l v_{rel} Substitute the expression for vrelv_{rel}: E=Bl8FSm\mathcal{E} = B l \sqrt{\frac{8FS}{m}} The current flowing through the resistor RR is given by Ohm's law: I=ER=BlR8FSmI = \frac{\mathcal{E}}{R} = \frac{B l}{R}\sqrt{\frac{8FS}{m}}

  7. Comparing with the given expression: The given expression for the current is I=BlRαFSmI = \frac{B l}{R}\sqrt{\frac{\alpha FS}{m}}. Comparing our derived expression with the given one: BlR8FSm=BlRαFSm\frac{B l}{R}\sqrt{\frac{8FS}{m}} = \frac{B l}{R}\sqrt{\frac{\alpha FS}{m}} From this, we can clearly see that α=8\alpha = 8.

The final answer is 8\boxed{8}.

Explanation of the solution:

  1. Identify that the net force on each rod is constant (Fnet=FF_{net} = F).
  2. Calculate the constant acceleration of each rod: a=F/ma = F/m.
  3. Determine the relative velocity (vrelv_{rel}) and total separation (xx) using constant acceleration kinematics: vrel=2atv_{rel} = 2at and x=at2x = at^2.
  4. Set the separation x=2Sx = 2S and solve for time tt: t=2SmFt = \sqrt{\frac{2Sm}{F}}.
  5. Substitute tt into the relative velocity expression to find vrelv_{rel} at separation 2S2S: vrel=8FSmv_{rel} = \sqrt{\frac{8FS}{m}}.
  6. Calculate the induced EMF: E=Blvrel\mathcal{E} = B l v_{rel}.
  7. Calculate the current: I=E/R=BlR8FSmI = \mathcal{E}/R = \frac{Bl}{R}\sqrt{\frac{8FS}{m}}.
  8. Compare this with the given current expression to find α=8\alpha = 8.