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There is one conducting circular loop of...

There is one conducting circular loop of radius R, which carries current I. There is another conducting circular loop of radius r placed coaxially at a distance x from it. Here `r lt lt R` and `x gt gt R`.
Magnetic flux linked smaller coil due to current in bigger coil is

A

`(mu_(0)IR^(2)pir^(2))/(2x^(3))`

B

`(mu_(0)IR^(2)pir^(2))/(x^(3))`

C

`(2mu_(0)IR^(2)pir^(2))/(x^(3))`

D

`(mu_(0)IR^(2)r^(2))/(4pix^(3))`

Text Solution

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The correct Answer is:
To solve the problem, we need to find the magnetic flux linked with the smaller coil due to the current in the larger coil. Here’s a step-by-step solution: ### Step 1: Find the Magnetic Field due to the Larger Coil The magnetic field \( B \) at a distance \( x \) from a circular loop of radius \( R \) carrying a current \( I \) can be calculated using the formula: \[ B = \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}} \] Given that \( x \gg R \), we can simplify this formula. Under this condition, \( R^2 + x^2 \approx x^2 \), so: \[ B \approx \frac{\mu_0 I R^2}{2x^3} \] ### Step 2: Calculate the Area of the Smaller Coil The area \( A \) of the smaller coil (which has a radius \( r \)) is given by: \[ A = \pi r^2 \] ### Step 3: Calculate the Magnetic Flux Linked with the Smaller Coil The magnetic flux \( \Phi \) linked with the smaller coil can be calculated using the formula: \[ \Phi = B \cdot A \] Substituting the expressions we derived for \( B \) and \( A \): \[ \Phi = \left(\frac{\mu_0 I R^2}{2x^3}\right) \cdot (\pi r^2) \] ### Step 4: Final Expression for the Magnetic Flux Thus, the magnetic flux linked with the smaller coil due to the current in the larger coil is: \[ \Phi = \frac{\mu_0 \pi I R^2 r^2}{2x^3} \] ### Summary The magnetic flux linked with the smaller coil is given by: \[ \Phi = \frac{\mu_0 \pi I R^2 r^2}{2x^3} \] ---

To solve the problem, we need to find the magnetic flux linked with the smaller coil due to the current in the larger coil. Here’s a step-by-step solution: ### Step 1: Find the Magnetic Field due to the Larger Coil The magnetic field \( B \) at a distance \( x \) from a circular loop of radius \( R \) carrying a current \( I \) can be calculated using the formula: \[ B = \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}} \] ...
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Knowledge Check

  • There is one conducting circular loop of radius R, which carries current I. There is another conducting circular loop of radius r placed coaxially at a distance x from it. Here r lt lt R and x gt gt R . Emf induced in the smaller loop when current in the bigger loop is changed at a rate of alpha is.

    A
    `(mu_(0)alphaR^(2)r^(2))/(2pix^(3))`
    B
    `(mu_(0)alphaR^(2)r^(2))/(2x^(3))`
    C
    `(2mu_(0)alphaR^(2)r^(2))/(x^(3))`
    D
    `(mu_(0)alphaR^(2)r^(2))/(4pix^(3))`
  • There is one conducting circular loop of radius R, which carries current I. There is another conducting circular loop of radius r placed coaxially at a distance x from it. Here r lt lt R and x gt gt R . Emf induced in the smaller loop when x starts increasing at a rate v.

    A
    `(3mu_(0)IvR^(2)r^(2))/(4pix^(4))`
    B
    `(6mu_(0)IvR^(2)r^(2))/(x^(4))`
    C
    `(3mu_(0)vR^(2)r^(2))/(2x^(4))`
    D
    `(3mu_(0)IvR^(2)r^(2))/(2pix^(4))`
  • A circular coil of radius 2R is carrying current I. The ratio of magnetic fields at the centre of coil and at a point at a distance 6R from centre of coil on axis of coil is

    A
    10
    B
    `10sqrt10`
    C
    `20sqrt5`
    D
    `20sqrt10`
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