A non-conducting ring having q uniformly distributed over its circumference is placed on a rough horizontal surface. A vertical time varying magnetic field `B = 4t^(2)` is switched on at time t = 0. Mass of the ring is m and radius is R.
The ring starts rotating after 2 s, the coefficient of friction between the ring and the table is
A non-conducting ring having q uniformly distributed over its circumference is placed on a rough horizontal surface. A vertical time varying magnetic field `B = 4t^(2)` is switched on at time t = 0. Mass of the ring is m and radius is R.
The ring starts rotating after 2 s, the coefficient of friction between the ring and the table is
The ring starts rotating after 2 s, the coefficient of friction between the ring and the table is
A
`(4qmR)/(g)`
B
`(2qmR)/(g)`
C
`(8qR)/(mg)`
D
`(qR)/(2mg)`
Text Solution
AI Generated Solution
The correct Answer is:
To solve the problem, we need to analyze the situation involving a non-conducting ring placed on a rough horizontal surface in a time-varying magnetic field. We will derive the expression for the coefficient of friction (μ) that allows the ring to start rotating after 2 seconds.
### Step-by-Step Solution:
1. **Identify the Magnetic Field and its Rate of Change**:
The magnetic field is given by \( B = 4t^2 \). To find the induced electromotive force (EMF), we first need to calculate the rate of change of the magnetic field:
\[
\frac{dB}{dt} = \frac{d}{dt}(4t^2) = 8t
\]
2. **Calculate the Induced EMF**:
The induced EMF (ε) in the ring can be calculated using Faraday's law of electromagnetic induction:
\[
\epsilon = -\frac{d\Phi}{dt}
\]
where \( \Phi \) is the magnetic flux. The area \( A \) of the ring is \( \pi R^2 \), thus:
\[
\Phi = B \cdot A = B \cdot \pi R^2 = 4t^2 \cdot \pi R^2
\]
Therefore, the induced EMF is:
\[
\epsilon = -\frac{d}{dt}(4t^2 \cdot \pi R^2) = -8t \cdot \pi R^2
\]
3. **Determine the Induced Electric Field**:
The induced electric field \( E \) can be related to the induced EMF by the formula:
\[
\epsilon = E \cdot (2\pi R)
\]
Thus, we can express the electric field as:
\[
E = \frac{\epsilon}{2\pi R} = \frac{-8t \cdot \pi R^2}{2\pi R} = -4tR
\]
4. **Calculate the Torque due to Electric Force**:
The electric force \( F \) acting on the charge \( q \) distributed uniformly on the ring due to the electric field is:
\[
F = qE = q(-4tR) = -4qtR
\]
The torque \( \tau \) caused by this force about the center of the ring is:
\[
\tau = F \cdot R = -4qtR^2
\]
5. **Calculate the Torque due to Friction**:
The torque due to friction \( \tau_f \) that opposes the motion is given by:
\[
\tau_f = \mu mgR
\]
6. **Set the Torques Equal at t = 2 seconds**:
The ring starts rotating at \( t = 2 \) seconds, so we set the magnitudes of the torques equal:
\[
4q(2)R^2 = \mu mgR
\]
7. **Solve for the Coefficient of Friction (μ)**:
Rearranging the equation gives:
\[
\mu = \frac{4q(2)R^2}{mgR} = \frac{8qR}{mg}
\]
### Final Expression for Coefficient of Friction:
\[
\mu = \frac{8qR}{mg}
\]
Similar Questions
Explore conceptually related problems
A conducting circular loop of radius a and resistance R is kept on a horizontal plane. A vertical time varying magnetic field B=2t is switched on at time t=0. Then
A non - conducting ring of mass m = 4 kg and radius R = 10 cm has charge Q = 2 C uniformly distributed over its circumference. The ring is placed on a rough horizontal surface such that the plane of the ring is parallel to the surface. A vertical magnetic field B=4t^(3)T is switched on at t = 0. At t = 5 s ring starts to rotate about the vertical axis through the centre. The coefficient of friction between the ring and the surface is found to be (k)/(24) . Then the value of k is
A non-conducting ring of mass m and radius R has a charge Q uniformly distributed over its circumference. The ring is placed on a rough horizontal surface such that plane of the ring is parallel to the surface. A vertical magnetic field B = B_0t^2 tesla is switched on. After 2 a from switching on the magnetic field the ring is just about to rotate about vertical axis through its centre. (a) Find friction coefficient mu between the ring and the surface. (b) If magnetic field is switched off after 4 s , then find the angle rotated by the ring before coming to stop after switching off the magnetic field.
A conducting ring of mass 2kg and radius 0.5m is placed on a smooth plane. The ring carries a current of i=4A . A horizontal magnetic field B=10 T is switched on at time t=0 as shown in fig The initial angular acceleration of the ring will be .
A conducting ring of mass 2kg and radius 0.5m is placed on a smooth plane. The ring carries a current of i=4A . A horizontal magnetic field B=10 T is switched on at time t=0 as shown in fig The initial angular acceleration of the ring will be .
A uniform conducting ring of mass pi kg and radius 1 m is kept on smooth horizontal table. A uniform but time varying magnetic field B = (hat (i) + t^(2) hat (j))T is present in the region, where t is time in seconds. Resistance of ring is 2 (Omega) . Then Heat generated (in kJ) through the ring till the instant when ring start toppling is
A conducting ring of mass 2kg, radius 0.5m carries a current of 4A. It is placed on a smooth horizontal surface. When a horizontal magnetic field of 10 T parallel to the diameter of the ring is applied, the initial acceleration is (in rad/se c^(2) )
A uniform conducting ring of mass pi kg and radius 1 m is kept on smooth horizontal table. A uniform but time varying magnetic field B = (hat (i) + t^(2) hat (j))T is present in the region, where t is time in seconds. Resistance of ring is 2 (Omega) . Then Time (in second) at which ring start toppling is
A uniform conducting ring of mass pi kg and radius 1 m is kept on smooth horizontal table. A uniform but time varying magnetic field B = (hat (i) + t^(2) hat (j))T is present in the region, where t is time in seconds. Resistance of ring is 2 (Omega) . Then Time (in second) at which ring start toppling is
Charge 'q' is uniformly distributed along the length of a non-coducting circular ring of mass m and radius 'a'. The ring is placed concentrically magnetic field B=kt (where k is constant) is existing perpendicular to the plane of circular region of radius 'R' as shown. The minimum coefficient of friction between the ring and the surface required to keep the ring stationary is
Recommended Questions
- A non-conducting ring having q uniformly distributed over its circumfe...
Text Solution
|
- A thin non conducting ring of mass m , radius a carrying a charge q ca...
Text Solution
|
- A non-conducting ring of mass m and radius R has a charge Q uniformly ...
Text Solution
|
- A ring of radius R is first rotated with an angular velocity omega and...
Text Solution
|
- A ring has a total mass M but non-uniformly distributed over its circu...
Text Solution
|
- There is a non-conducting disc of mass 4kg and radius 1m placed on a r...
Text Solution
|
- A non-conducting ring having q uniformly distributed over its circumfe...
Text Solution
|
- A ring of mass m, radius r having charge q uniformly distributed over ...
Text Solution
|
- A non - conducting ring of mass m = 4 kg and radius R = 10 cm has char...
Text Solution
|