Physics, asked by renusachdeva9788, 1 year ago

Find the magnetic field B at the centre of a rectangular loop of length l and width b, carrying a current i.

Answers

Answered by gauravarduino
0

Explanation:

Find the magnetic field B at the centre of a rectangular loop of length l and width b, carrying a current i. =2μoi√b2+l2πbl. CBSE to introduce major changes in exam pattern of Class 10 and Class 12 board classes by 2023. Get here complete updates on the CBSE 2020 exam.

Answered by bhuvna789456
2

The magnetic field B at the centre of a rectangular loop of length l and width b, carrying a current i is given by \frac{2 \mu_{0} i \sqrt{b^{2}+l^{2}}}{\pi l b} .

Explanation:

Step 1:

Let \theta_1 and \theta_2 , respectively, be the angles of points A and B with point O.

\theta_1 = \theta_2 = θ  

Divide the point from wire, d = \frac{b}{2}

In case of  ∆AOM,

A O=\sqrt{\left(\frac{b}{2}\right)^{2}+\left(\frac{l}{2}\right)^{2}}=\frac{1}{2} \sqrt{b^{2}+l^{2}}

\sin \theta=\frac{\frac{l}{2}}{\frac{1}{2} \sqrt{b^{2}+l^{2}}}=\frac{1}{\sqrt{b^{2}+l^{2}}}

Step 2:

Therefore, the current magnetic field in wire AB is given by

B=\frac{\mu_{0} i}{4 \pi d}\left(\sin \theta_{1}+\sin \theta_{2}\right)

B=\frac{\mu_{0} t}{4 \pi d} \times 2 \sin \theta

B=\frac{\mu_{0} i}{4 \pi \frac{b}{2}} \times \frac{2 l}{\sqrt{b^{2}+l^{2}}}

  =\frac{\mu_{0} i}{\pi b} \times \frac{l}{\sqrt{b^{2}+l^{2}}}

Step 3:

Likewise, due to current in wire BC the magnetic field is given by

b^{\prime}=\frac{\mu_{0} i}{\pi l} \times \frac{b}{\sqrt{b^{2}+l^{2}}}

Current magnetic field in wire CD = Magnetic field due to current in wire AB = B  

And,  

Current in wire DA = Magnetic field due to current in wire BC = B '

b^{\prime}=\frac{\mu_{0} i}{\pi l} \times \frac{b}{\sqrt{b^{2}+l^{2}}}

  =2\left[\frac{\mu_{0} i}{\pi b} \times \frac{l}{\sqrt{b^{2}+l^{2}}}+\frac{\mu_{0} i}{\pi l} \times \frac{b}{\sqrt{b^{2}+l^{2}}}\right]

   =2 \frac{\mu_{0} i}{\pi \sqrt{b^{2}+l^{2}}} \times\left[\frac{l}{b}+\frac{b}{l}\right]

  =\frac{2 \mu_{0} i \sqrt{b^{2}+l^{2}}}{\pi l b}

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