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A non - conducting ring of mass m = 4 kg...

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

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To solve the problem, we will follow these steps: ### Step 1: Calculate the Magnetic Flux (Φ) The magnetic field is given as \( B = 4t^3 \, \text{T} \). The area \( A \) of the ring is given by: \[ A = \pi R^2 \] where \( R = 0.1 \, \text{m} \) (10 cm converted to meters). Thus, \[ A = \pi (0.1)^2 = \pi (0.01) = 0.01\pi \, \text{m}^2 \] The magnetic flux \( \Phi \) through the ring is: \[ \Phi = B \cdot A = (4t^3) \cdot (0.01\pi) = 0.04\pi t^3 \] ### Step 2: Calculate the EMF (Electromotive Force) Using Faraday's law of electromagnetic induction, the EMF \( \mathcal{E} \) induced in the ring is given by: \[ \mathcal{E} = -\frac{d\Phi}{dt} \] Calculating the derivative: \[ \mathcal{E} = -\frac{d}{dt}(0.04\pi t^3) = -0.12\pi t^2 \] ### Step 3: Calculate the EMF at \( t = 5 \, \text{s} \) Substituting \( t = 5 \): \[ \mathcal{E} = -0.12\pi (5^2) = -0.12\pi (25) = -3\pi \, \text{V} \] ### Step 4: Calculate the Force on the Ring The force \( F \) acting on the ring due to the electric field generated by the EMF is: \[ F = Q \cdot \mathcal{E} \] where \( Q = 2 \, \text{C} \): \[ F = 2 \cdot (3\pi) = 6\pi \, \text{N} \] ### Step 5: Relate the Force to Friction The frictional force \( F_f \) that prevents the ring from sliding is given by: \[ F_f = \mu mg \] where \( m = 4 \, \text{kg} \) and \( g = 10 \, \text{m/s}^2 \): \[ F_f = \mu (4)(10) = 40\mu \] ### Step 6: Set the Forces Equal At the moment the ring starts to rotate, the force due to the EMF equals the frictional force: \[ 6\pi = 40\mu \] Thus, \[ \mu = \frac{6\pi}{40} = \frac{3\pi}{20} \] ### Step 7: Relate Coefficient of Friction to \( k \) We know from the problem statement that: \[ \mu = \frac{k}{24} \] Setting the two expressions for \( \mu \) equal gives: \[ \frac{3\pi}{20} = \frac{k}{24} \] ### Step 8: Solve for \( k \) Cross-multiplying to solve for \( k \): \[ 3\pi \cdot 24 = 20k \] \[ k = \frac{72\pi}{20} = \frac{18\pi}{5} \] ### Step 9: Approximate \( k \) Using \( \pi \approx 3.14 \): \[ k \approx \frac{18 \cdot 3.14}{5} \approx \frac{56.52}{5} \approx 11.30 \] ### Conclusion The value of \( k \) is approximately \( 11.30 \).
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