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BITSAT 2015
Exam
BITSAT
Year
2015
Subject
Physics
Chapter
Magnetic Effects of Current

BITSAT 2015 · Physics · Magnetic Effects of Current

A long straight wire along the Z -axis carries a current I in the...

A long straight wire along the ZZ -axis carries a current I in the negative ZZ -direction. The magnetic vector field B⃗\vec{B} at a point having coordinates (x,y)(x, y) in the Z=0Z=0 plane isA long straight wire along the Z -axis carries a current I in the negative Z -direction. The magnetic vector field B at

Options

  1. A\frac{\mu_{0} I(y \hat{i}-x \hat{j})}{2 \pi\left(x^{2}+y^{2}\right)}
  2. B\frac{\mu_{0} I(x \hat{i}+y \hat{j})}{2 \pi\left(x^{2}+y^{2}\right)}
  3. C\frac{\mu_{0} I(x \hat{j}-y \hat{i})}{2 \pi\left(x^{2}+y^{2}\right)}
  4. D\frac{\mu_{0} I(x \hat{i}-y \hat{j})}{2 \pi\left(x^{2}+y^{2}\right)}

Correct answer

A. \frac{\mu_{0} I(y \hat{i}-x \hat{j})}{2 \pi\left(x^{2}+y^{2}\right)}

Step-by-step solution

The wire carries a current II in the negative zz -direction. We have to consider the magnetic vector field B⃗\vec{B} at (x,y)(x, y) in the z=0z=0 plane. A long straight wire along the Z -axis carries a current I in the negative Z -direction. The magnetic vector field B at
Magnetic field B⃗\vec{B} is perpendicular to OP∴B⃗=Bsin⁡θi^−Bcos⁡θj^O P\therefore \vec{B}=B \sin \theta \hat{i}-B \cos \theta \hat{j}sin⁡θ=yr,cos⁡θ=xrB=μ0I2πr∴B⃗=μ0I2πr2(yi^−xj^)\begin{array}{l} \sin \theta=\frac{y}{r}, \cos \theta=\frac{x}{r}B=\frac{\mu_{0} I}{2 \pi r}\\ \therefore \quad \vec{B}=\frac{\mu_{0} I}{2 \pi r^{2}}( y \hat{i}-x \hat{j}) \end{array}oror\quad $\vec{B}=\frac{\mu_{0} I(y \hat{i}-x \hat{j})}{2 \pi \left(x^{2}+y^{2}\right)}
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