A long wire carrying a current of 5 A lies along the positive Z-axis. The magnetic field the point with position vector \(\vec{r}\) =(\(\hat{i}\)+2\(\hat{j}\)+2\(\hat{k}\)) m will be:(μo=4\(\pi\)×10-7 in SI units)
2\(\sqrt{5}\)x10-7 T
5x10-7 T
0.33x10-7 T
0.66x10-7 T
7\(\sqrt{5}\) x10-7 T
The correct answer is (A): 2\(\sqrt{5}\)x10-7 T
\(B=\frac{μ_0I}{2πr}\)
where:
Given the position vector\(r=\^{r}+2\^{j}+2\^{k}\) m, we need to find the perpendicular distance from this point to the wire, which lies along the positive z-axis.
Since the wire is along the z-axis, the distance is the magnitude of the projection of r onto the xy-plane, which is given by the vector 𝑟𝑥𝑦= \(\^i+2\^j\)
The magnitude of rxy is:
\(r=\sqrt{(1)^2+(2)^2=\sqrt{1+4}}=\sqrt5m\)
Now we substitute the values into the equation for the magnetic field:
\(B=\frac{μ_0I}{2πr}\) = \(\frac{(4\pi\times10^{-7})\times5}{2\pi\sqrt5}\)=\(=\frac{20\pi\times10^{-7}}{2\pi\sqrt5}\)=\(=\frac{20\times10^{-7}}{2\sqrt5}\) \(=\frac{10\times10^{-7}}{\sqrt5}\)
=\(2 \times10^{-7}\sqrt5\)
Thus, the magnetic field at the point \(r=\^i+2\^j+2\^k\) is:
\(B=2\sqrt2\times10^{-7} T\)
Biot-Savart’s law is an equation that gives the magnetic field produced due to a current-carrying segment. This segment is taken as a vector quantity known as the current element. In other words, Biot-Savart Law states that if a current carrying conductor of length dl produces a magnetic field dB, the force on another similar current-carrying conductor depends upon the size, orientation and length of the first current carrying element.
The equation of Biot-Savart law is given by,
\(dB = \frac{\mu_0}{4\pi} \frac{Idl sin \theta}{r^2}\)
For detailed derivation on Biot Savart Law, read more.