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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Magnetic Field due to a Current

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Magnetic Field due to a Current

An idealized magnetic field that is uniform within a specific...

An idealized magnetic field that is uniform within a specific region and abruptly drops to zero is sometimes depicted, as illustrated in the figure. By applying Ampere's law along the path PQRSPQRS, identify the reason why such a field configuration is impossible.
An idealized magnetic field that is uniform within a specific region and abruptly drops to zero is sometimes depicted,

Options

  1. AAmpere's law is only applicable to non-uniform magnetic fields and cannot be evaluated along the chosen path.
  2. BThe line integral ∮B⃗⋅dl⃗\oint \vec{B} \cdot d\vec{l} over the loop PQRSPQRS is exactly zero, whereas the enclosed current is non-zero.
  3. CThe line integral ∮B⃗⋅dl⃗\oint \vec{B} \cdot d\vec{l} over the loop PQRSPQRS evaluates to a non-zero value, whereas the enclosed current is zero.
  4. DThe line integral ∮B⃗⋅dl⃗\oint \vec{B} \cdot d\vec{l} is mathematically undefined at the boundary where the magnetic field abruptly drops to zero.

Correct answer

C. The line integral ∮B⃗⋅dl⃗\oint \vec{B} \cdot d\vec{l} over the loop PQRSPQRS evaluates to a non-zero value, whereas the enclosed current is zero.

Step-by-step solution

Consider the rectangular Amperian loop PQRSPQRS.

The line integral of the magnetic field along the loop is given by:

∮B⃗⋅dl⃗=∫PQB⃗⋅dl⃗+∫QRB⃗⋅dl⃗+∫RSB⃗⋅dl⃗+∫SPB⃗⋅dl⃗\oint \vec{B} \cdot d\vec{l} = \int_P^Q \vec{B} \cdot d\vec{l} + \int_Q^R \vec{B} \cdot d\vec{l} + \int_R^S \vec{B} \cdot d\vec{l} + \int_S^P \vec{B} \cdot d\vec{l}

Along the paths PQPQ and RSRS, the magnetic field B⃗\vec{B} is perpendicular to the path elements dl⃗d\vec{l}, so B⃗⋅dl⃗=0\vec{B} \cdot d\vec{l} = 0.

Along the path QRQR, the magnetic field is zero, so ∫QRB⃗⋅dl⃗=0\int_Q^R \vec{B} \cdot d\vec{l} = 0.

Along the path SPSP, the magnetic field B⃗\vec{B} is uniform and parallel to dl⃗d\vec{l}. Let the length of SPSP be ll. Then ∫SPB⃗⋅dl⃗=Bl\int_S^P \vec{B} \cdot d\vec{l} = Bl.

Therefore, the total line integral is ∮B⃗⋅dl⃗=Bl≠0\oint \vec{B} \cdot d\vec{l} = Bl \neq 0.

However, the current enclosed by the loop PQRSPQRS is zero (Ienclosed=0I_{enclosed} = 0).

According to Ampere's law, ∮B⃗⋅dl⃗=μ0Ienclosed\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{enclosed}. This would require Bl=0Bl = 0, which contradicts the presence of a uniform magnetic field.

Thus, such a field configuration is impossible because the line integral evaluates to a non-zero value, whereas the enclosed current is zero.
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