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Question: ماهي محصلة كثافة الفيض المغناطيسي عند مركز الحلقة (c)؟...

ماهي محصلة كثافة الفيض المغناطيسي عند مركز الحلقة (c)؟

A

8×106T8 \times 10^{-6} T

B

3.2×105T3.2 \times 10^{-5} T

C

4×106T4 \times 10^{-6} T

D

1.6×105T1.6 \times 10^{-5} T

Answer

8×106T8 \times 10^{-6} T

Explanation

Solution

The problem asks for the net magnetic field at the center (c) of a circular metallic loop. The setup involves two sources of magnetic fields:

  1. A circular loop with current entering at point x and leaving at point y.
  2. A straight wire tangent to the loop, carrying a current of 2A.

1. Magnetic field due to the circular loop:

The current II enters the loop at point x and leaves at point y. This means the current divides into two paths: one through the minor arc (between x and y) and another through the major arc (between x and y).

Since the magnetic fields B1B_1 and B2B_2 have equal magnitudes and opposite directions (one into the page, one out of the page), the net magnetic field due to the circular loop at its center is: Bloop=B1B2=0B_{loop} = B_1 - B_2 = 0.

This is a general result: for a current-carrying loop where current enters and leaves at two points, the net magnetic field at the center is always zero.

2. Magnetic field due to the straight wire:

The straight wire is tangent to the top of the loop and carries a current of 2A2A. The average diameter of the loop is 10 cm, so its radius is r=10 cm2=5 cm=0.05 mr = \frac{10 \text{ cm}}{2} = 5 \text{ cm} = 0.05 \text{ m}. Since the wire is tangent to the loop, the perpendicular distance from the center 'c' to the straight wire is equal to the radius of the loop, d=r=0.05 md = r = 0.05 \text{ m}.

The magnetic field due to a long straight current-carrying wire is given by: Bwire=μ0Iwire2πdB_{wire} = \frac{\mu_0 I_{wire}}{2\pi d} Given μ0=4π×107 Wb/A.m\mu_0 = 4\pi \times 10^{-7} \text{ Wb/A.m} and Iwire=2 AI_{wire} = 2 \text{ A}. Bwire=(4π×107 Wb/A.m)×(2 A)2π×(0.05 m)=8×106 TB_{wire} = \frac{(4\pi \times 10^{-7} \text{ Wb/A.m}) \times (2 \text{ A})}{2\pi \times (0.05 \text{ m})} = 8 \times 10^{-6} \text{ T}.

3. Net magnetic field at center 'c':

The net magnetic field at the center 'c' is the vector sum of the fields due to the loop and the straight wire: Bnet=Bloop+BwireB_{net} = B_{loop} + B_{wire} Since Bloop=0B_{loop} = 0, Bnet=Bwire=8×106 TB_{net} = B_{wire} = 8 \times 10^{-6} \text{ T}.