A rectangular loop and a circular loop are moving out of a uniform magnetic field region (as shown in the figure) to a field-free region with a constant velocity \(v.\) In which loop do you expect the induced emf to be constant during the passage out of the field region? The field is normal to the loops:

   

1. only in the case of the rectangular loop
2. only in the case of the circular loop

3. in both cases

4. none of these

Subtopic:  Faraday's Law & Lenz Law |
 65%
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The polarity of the capacitor in the given figure is:

     

1. The polarity of plate \(B\) will be positive with respect to plate \(A.\)
2. The polarity of plate \(A\) will be positive with respect to plate \(B.\)
3. The polarity of plate \(A\) will be the same as that of plate \(B.\)
4. None of these
Subtopic:  Faraday's Law & Lenz Law |
 64%
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A metallic rod of \(1 ~\text m\) length is rotated with a frequency of \(50 ~\text{rev/s},\) with one end hinged at the centre and the other end at the circumference of a circular metallic ring of radius \(1 ~\text m,\) about an axis passing through the centre and perpendicular to the plane of the ring (as shown in the figure). A constant and uniform magnetic field of \(1 ~\text T\) parallel to the axis is present everywhere. What is the emf between the centre and the metallic ring?

   
1. \(150 ~\text V\)
2. \(130 ~\text V\)
3. \(157 ~\text V\)
4. \(133 ~\text V\)

Subtopic:  Motional emf |
 74%
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A wheel with \(10\) metallic spokes each \(0.5~\text{m}\) long is rotated with a speed of \(120~\text{rev/min}\) in a plane normal to the horizontal component of Earth’s magnetic field \(H_E\) at a place. If \(H_E=0.4~\text{G}\) at the place, what is the induced emf between the axle and the rim of the wheel? (\((1~\text{G}=10^{-4}~\text{T})\) 
1. \(5.12\times10^{-5}~\text{V}\) 
2. \(0\)
3. \(3.33\times10^{-5}~\text{V}\)
4. \(6.28\times10^{-5}~\text{V}\)

Subtopic:  Motional emf |
 66%
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Refer to figure. The arm \(PQ\) of the rectangular conductor is moved from \(x = 0,\) outwards. The uniform magnetic field is perpendicular to the plane and extends from \(x = 0\) to \(x = b\) and is zero for \(x > b.\) Only the arm \(PQ\) possesses substantial resistance \(r.\) Consider the situation when the arm \(PQ\) is pulled outwards from \(x = 0\) to \(x = 2b\) with a` constant speed \(v.\) The induced emf is:

  

1. \(- Blv   ~\text{for }~  0 \leq x < b ,~~~   0   ~\text{for}~   b \leq x < 2 b\)
2. \(  + Blv   ~\text{for}~   0 \leq x < b ,   ~~~0   ~\text{for }~  b \leq x < 2 b\)
3. \(- Blv   ~\text{for}~   b \leq x < 2 b ,  ~~~0 ~\text{for }~  0 \leq x < b\)
4. \(+ Blv  ~\text{for}  ~ b \leq x < 2 b , ~~~  0  ~\text{for}~   0 \leq x < b\)

Subtopic:  Motional emf |
 52%
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Refer to the figure, the arm \(PQ\) of the rectangular conductor is moved from \(x=0,\) outwards. The uniform magnetic field is perpendicular to the plane and extends from \(x=0~to~x=b\) to \(x=b\) and is zero for \(x>b.\) Only the arm \(PQ\) possesses substantial resistance \(r.\) Consider the situation when the arm \(PQ\) is pulled outwards from \( x = 0  \) to \(x=2b\) with constant speed \(v.\) The force necessary to pull the arm is:

1. \(~\dfrac{B^2l^2v}{r}~\text{for}~0\leq x<b,~0~\text{for}~b\leq x<2b\)
2. \(~\dfrac{B^2l^2v}{2r}~\text{for}~0\leq x<b,~0~\text{for}~b\leq x<2b\)
3. \(~0~\text{for}~0\leq x<b,~\dfrac{B^2l^2v}{r}~\text{for}~b\leq x<2b\)
4. \(~0~\text{for}~0\leq x<b,~\dfrac{B^2l^2v}{2r}~\text{for}~b\leq x<2b\)
Subtopic:  Motional emf |
 76%
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The arm \(PQ\) of the rectangular conductor is moved from \(x = 0,\) outwards. The uniform magnetic field is perpendicular to the plane and extends from \(x = 0\) to \(x = b\) and is zero for \(x > b.\) Only the arm \(PQ\) possesses substantial resistance \(r.\) Consider the situation when the arm \(PQ\) is pulled outwards from \(x = 0\) to \(x = 2b\) and is then moved back to \(x = 0\) with constant speed \(v.\) The power dissipated as Joule heat is: 

                

1. \(\dfrac{{B}^2 {l}^2 {v}}{2{r}}~~\text{for}~0 \leq {x}<{b},~~~ 0~~\text{for} ~{b} \leq {x}<2 {b}\)
2. \(\dfrac{{B}^2 {l}^2 {v^2}}{{r}}~~\text{for}~0 \leq {x}<{b},~~~ 0~~\text{for} ~{b} \leq {x}<2 {b}\)
3. \(0~~\text{for}~b \leq {x}<{2b},~~~ \dfrac{{B}^2 {l}^2 {v}^2}{{r}}~~\text{for} ~{0} \leq {x}< {b}\)
4. \(0~~\text{for}~b \leq {x}<{2b},~~~ \dfrac{{B}^2 {l}^2 {v}}{{2r}}~~\text{for} ~{0} \leq {x}< {b}\)
Subtopic:  Motional emf |
 76%
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Two concentric circular coils, one of small radius \({r_1}\) and the other of large radius \({r_2},\) such that \({r_1<<r_2},\)  are placed co-axially with centres coinciding. The mutual inductance of the arrangement is:
1. \(\dfrac{\mu_0\pi r_1^2}{3r_2}\)


2. \(\dfrac{2\mu_0\pi r_1^2}{r_2}\)

3. \(\dfrac{\mu_0\pi r_1^2}{r_2}\)

4. \(\dfrac{\mu_0\pi r_1^2}{2r_2}\)

Subtopic:  Mutual Inductance |
 70%
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The expression for the magnetic energy stored in a solenoid in terms of magnetic field \(B\), area \(A\) and length \(l\) of the solenoid is:

1. \( \dfrac{1}{\mu_0}B^2Al\) 2. \( \dfrac{1}{2\mu_0}B^2Al\)
3. \( \dfrac{2}{\mu_0}B^2Al\) 4. \( \dfrac{3}{2\mu_0}B^2Al\)
Subtopic:  Self - Inductance |
 84%
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The ratio of magnetic energy per unit volume and electrostatic energy stored per unit volume in a parallel plate capacitor is:
1. \(\left(\dfrac{1}{\varepsilon_0 \mu_0}\right)\dfrac{B^2}{E}\)

2. \(\left(\dfrac{1}{\varepsilon_0 \mu_0}\right)\dfrac{E^2}{B}\)

3. \(\left(\dfrac{1}{2\varepsilon_0 \mu_0}\right)\dfrac{B^2}{E}\)

4. \(\left(\dfrac{1}{2\varepsilon_0 \mu_0}\right)\dfrac{E^2}{B}\)

Subtopic:  Self - Inductance |
 64%
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