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JEE MainPhysicsToughMagnetic effects of current

A very long wire ABDMNDC is shown in figure carrying current I.
AB and BC parts are straight, longand at right angle. At D wire forms a

circular turn DMND of radius R. AB, BC parts are tangential tocircular

turn at N and D. Magnetic field at the centre of circle is

Show answer and solution
μ0i4πR[sin⁡90∘−sin⁡45∘]⊗+μ0i2R⊙+μ0i4πR(sin⁡45∘+sin⁡90∘)⊙\frac{\mu_{0}i}{4\pi R}\left\lbrack \sin 90^{\circ} - \sin 45^{\circ} \right\rbrack \otimes + \frac{\mu_{0}i}{2R} \odot + \frac{\mu_{0}i}{4\pi R}\left( \sin 45^{\circ} + \sin 90^{\circ} \right) \odot
=−μ0i4πR[1−12]+μ0j2R+μ0i4πR[12+1]⊙= \frac{- \mu_{0}i}{4\pi R}\left\lbrack 1 - \frac{1}{\sqrt{2}} \right\rbrack + \frac{\mu_{0}j}{2R} + \frac{\mu_{0}i}{4\pi R}\left\lbrack \frac{1}{\sqrt{2}} + 1 \right\rbrack \odot
=μ0i4πR[−1+12+2π+12+1]⊙= \frac{\mu_{0}i}{4\pi R}\left\lbrack - 1 + \frac{1}{\sqrt{2}} + 2\pi + \frac{1}{\sqrt{2}} + 1 \right\rbrack \odot
=μ0i4πR[2+2π]⊙= \frac{\mu_{0}i}{4\pi R}\lbrack\sqrt{2} + 2\pi\rbrack \odot
=μ0i2πR[12+π]⊙= \frac{\mu_{0}i}{2\pi R}\left\lbrack \frac{1}{\sqrt{2}} + \pi \right\rbrack \odot

Source: Grass-G / P-13 Physics paper 4 Nov.docx

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