Home
Class 12
PHYSICS
A uniform conducting ring of mass m=2kg,...

A uniform conducting ring of mass `m=2kg`, radius `r=2m` and resistance `8Omega` is kept on smooth, horizontal surface. A time varying magnetic field `vecB=(hati+t^(2)hatj)` Tesla is present in the region, where `t` is time in second and take vertical as `y`-axis. (Take `pi^(2)=10`). Then

A

Time when ring starts toppling is 1/2 sec

B

Time when ring starts toppling is `3//4` sec

C

Heat generated through the ring till the instant when the ring start toppling is `40//3` Joule.

D

Heat generated through the ring till the instant when the ring start toppling is `80//3` Joule

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to determine the time when the conducting ring starts to topple due to the induced current in the presence of a time-varying magnetic field. We will analyze the torques acting on the ring due to its weight and the magnetic field. ### Step-by-Step Solution: 1. **Identify the Forces and Torques:** - The ring has a mass \( m = 2 \, \text{kg} \). - The weight of the ring \( F_w = mg = 2 \times 10 = 20 \, \text{N} \) acts downwards. - The torque due to the weight \( \tau_w \) is given by: \[ \tau_w = r \times F_w = 2 \, \text{m} \times 20 \, \text{N} = 40 \, \text{N m} \] 2. **Calculate the Magnetic Flux:** - The magnetic field is given by \( \vec{B} = \hat{i} + t^2 \hat{j} \). - The area \( A \) of the ring is \( A = \pi r^2 = \pi (2^2) = 4\pi \, \text{m}^2 \). - The magnetic flux \( \Phi \) through the ring is: \[ \Phi = \int \vec{B} \cdot d\vec{A} = \int (1 \hat{i} + t^2 \hat{j}) \cdot (0 \hat{i} + 1 \hat{j}) \, dA = 4\pi t^2 \] 3. **Calculate the Induced EMF:** - The induced EMF \( \mathcal{E} \) is given by: \[ \mathcal{E} = -\frac{d\Phi}{dt} = -\frac{d}{dt}(4\pi t^2) = -8\pi t \] 4. **Calculate the Induced Current:** - The resistance \( R \) of the ring is \( 8 \, \Omega \). - The induced current \( I \) is given by: \[ I = \frac{\mathcal{E}}{R} = \frac{-8\pi t}{8} = -\pi t \] 5. **Calculate the Force due to the Magnetic Field:** - The force \( F_B \) on the ring due to the magnetic field is given by: \[ F_B = I A \times \vec{B} = (-\pi t)(4\pi) \hat{j} \times (\hat{i} + t^2 \hat{j}) = -4\pi^2 t \hat{k} \] 6. **Calculate the Torque due to the Magnetic Field:** - The torque \( \tau_B \) due to the magnetic field is: \[ \tau_B = r \times F_B = 2 \, \hat{r} \times (-4\pi^2 t \hat{k}) = 8\pi^2 t \, \text{N m} \] 7. **Set the Torques Equal to Find the Time:** - The ring will start to topple when the torque due to the magnetic field equals the torque due to the weight: \[ \tau_B = \tau_w \implies 8\pi^2 t = 40 \] - Substituting \( \pi^2 = 10 \): \[ 80t = 40 \implies t = \frac{1}{2} \, \text{s} \] ### Final Answer: The time when the ring starts to topple is \( t = \frac{1}{2} \, \text{s} \).

To solve the problem, we need to determine the time when the conducting ring starts to topple due to the induced current in the presence of a time-varying magnetic field. We will analyze the torques acting on the ring due to its weight and the magnetic field. ### Step-by-Step Solution: 1. **Identify the Forces and Torques:** - The ring has a mass \( m = 2 \, \text{kg} \). - The weight of the ring \( F_w = mg = 2 \times 10 = 20 \, \text{N} \) acts downwards. - The torque due to the weight \( \tau_w \) is given by: ...
Promotional Banner

Similar Questions

Explore conceptually related problems

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

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 Net Induced EMF (in Volt) on conducting ring as function of time 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 Heat generated (in kJ) through the ring till the instant when ring start toppling is

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 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 conducting ring of radius r and resistance R is placed in region of uniform time varying magnetic field B which is perpendicular to the plane of the ring. It the magnetic field is changing at a rate alpha , then the current induced in the ring 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

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 circular conducting coil of radius T_0 , having resistance R is placed in a time varying transverse uniform magnetic field B=4t^2 as shown in the figure. The current in the coil at time t = 2 s is (consider all quantities are in Si units)