Numerical Problems Based on Biot-Savart Law for Class 12 Physics

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Numerical Problems on Biot-Savart Law

Class 12 Physics · Moving Charges and Magnetism
SQ

Biot-Savart Law Practice Set

Apply $d\vec{B} = \frac{\mu_0}{4\pi} \frac{I d\vec{l} \times \hat{r}}{r^2}$
Ch 4 · Moving Charges and Magnetism
1
A wire placed along east-west direction carries a current of 10 A from west to east direction. Determine the magnetic field due to a 1.8 cm piece of wire at a point 300 cm north-east from the piece.
Answer $1.4 \times 10^{-9}\text{ T}$, normally out of the plane of paper 📝
Detailed Solution

Given parameters: Current $I = 10\text{ A}$, length of element $dl = 1.8\text{ cm} = 1.8 \times 10^{-2}\text{ m}$, distance $r = 300\text{ cm} = 3\text{ m}$.

The current flows from West to East. The point is North-East, so the angle $\theta$ between the current element and the position vector is $45^\circ$.

According to the Biot-Savart Law:

$$dB = \frac{\mu_0}{4\pi} \frac{I dl \sin\theta}{r^2}$$

Substitute the values (where $\frac{\mu_0}{4\pi} = 10^{-7}\text{ T m/A}$):

$$dB = 10^{-7} \times \frac{10 \times 1.8 \times 10^{-2} \times \sin(45^\circ)}{(3)^2}$$
$$dB = 10^{-7} \times \frac{0.18 \times (1/\sqrt{2})}{9} = 10^{-7} \times 0.02 \times 0.707$$
$$dB \approx 1.414 \times 10^{-9}\text{ T}$$

Applying the Right-Hand Thumb Rule, curling fingers from the East vector towards the North-East vector gives a direction pointing normally out of the plane of paper.

2
A small current element $I d\vec{l}$, with $d\vec{l} = 2\hat{k}\text{ mm}$ and $I = 2\text{ A}$ is centred at the origin. Find magnetic field $d\vec{B}$ at the following points:
(i) On the x-axis at $x = 3\text{ m}$.
(ii) On the x-axis at $x = -6\text{ m}$.
(iii) On the z-axis at $z = 3\text{ m}$.
Answer (i) $4.44 \times 10^{-11} \hat{j}\text{ T}$ (ii) $-1.11 \times 10^{-11} \hat{j}\text{ T}$ (iii) 0 📝
Detailed Solution

Given current element $I d\vec{l} = 2(2 \times 10^{-3}\hat{k}) = 4 \times 10^{-3}\hat{k}\text{ Am}$.

The vector form of the Biot-Savart Law is $d\vec{B} = \frac{\mu_0}{4\pi} \frac{I d\vec{l} \times \vec{r}}{r^3}$ or $d\vec{B} = \frac{\mu_0}{4\pi} \frac{I d\vec{l} \times \hat{r}}{r^2}$.

(i) At $x = 3\text{ m}$ ($\vec{r} = 3\hat{i}$, $r = 3\text{ m}$):

$$d\vec{B} = 10^{-7} \frac{(4 \times 10^{-3}\hat{k}) \times (3\hat{i})}{3^3} = 10^{-7} \frac{12 \times 10^{-3}(\hat{k} \times \hat{i})}{27}$$

Since $\hat{k} \times \hat{i} = \hat{j}$:

$$d\vec{B} = 10^{-10} \times \frac{12}{27} \hat{j} \approx 4.44 \times 10^{-11} \hat{j}\text{ T}$$

(ii) At $x = -6\text{ m}$ ($\vec{r} = -6\hat{i}$, $r = 6\text{ m}$):

$$d\vec{B} = 10^{-7} \frac{(4 \times 10^{-3}\hat{k}) \times (-6\hat{i})}{6^3} = 10^{-7} \frac{-24 \times 10^{-3}(\hat{k} \times \hat{i})}{216}$$
$$d\vec{B} = 10^{-10} \times \frac{-24}{216} \hat{j} \approx -1.11 \times 10^{-11} \hat{j}\text{ T}$$

(iii) At $z = 3\text{ m}$ ($\vec{r} = 3\hat{k}$, $r = 3\text{ m}$):

Here, $d\vec{l}$ is along $\hat{k}$ and $\vec{r}$ is also along $\hat{k}$. The angle between them is $0^\circ$.

$$\hat{k} \times \hat{k} = 0 \implies d\vec{B} = 0$$
3

An element $\Delta\vec{l} = \Delta x \hat{i}$ is placed at the origin (as shown in Fig. 4.6) and carries a current $I = 2\text{ A}$. Find out the magnetic field at a point P on the y-axis at a distance of 1.0 m due to the element $\Delta x = 1\text{ cm}$. Give also the direction of the field produced.

Answer $2 \times 10^{-9}\text{ T}$, in $+z$-direction 📝
Detailed Solution

Given parameters:
Current $I = 2\text{ A}$.
Element vector $\Delta\vec{l} = \Delta x \hat{i} = 1\text{ cm } \hat{i} = 10^{-2} \hat{i}\text{ m}$.
Position vector of point P on the y-axis, $\vec{r} = 1.0 \hat{j}\text{ m}$. Distance $r = 1.0\text{ m}$.

Using the vector form of Biot-Savart Law:

$$\Delta\vec{B} = \frac{\mu_0}{4\pi} \frac{I (\Delta\vec{l} \times \vec{r})}{r^3}$$

Substitute the values:

$$\Delta\vec{B} = 10^{-7} \times \frac{2 \times (10^{-2}\hat{i} \times 1.0\hat{j})}{(1.0)^3}$$
$$\Delta\vec{B} = 2 \times 10^{-9} (\hat{i} \times \hat{j})$$

Since the cross product $\hat{i} \times \hat{j} = \hat{k}$:

$$\Delta\vec{B} = 2 \times 10^{-9} \hat{k}\text{ T}$$

The magnitude is $2 \times 10^{-9}\text{ T}$ and the direction is along the $+z$-axis.

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