Numerical Problems Based on Ampere’s Circuital Law for Class 12 Physics

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Numerical Problems on Ampere’s Circuital Law

Class 12 Physics · Moving Charges and Magnetism
SQ

Ampere’s Law and Solenoids Practice Set

Apply $\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{enclosed}$ and solenoid/toroid formulas
Ch 4 · Moving Charges and Magnetism
1
A long solenoid consists of 20 turns per cm. What current is necessary to produce a magnetic field of 20 mT inside the solenoid?
Answer 8.0 A 📝
Detailed Solution

Given parameters: Magnetic field $B = 20\text{ mT} = 20 \times 10^{-3}\text{ T}$.

Turn density ($n$) must be converted to turns per meter:

$$n = 20\text{ turns/cm} = 2000\text{ turns/m}$$

Using the formula for the magnetic field inside a long solenoid $B = \mu_0 n I$, solve for current ($I$):

$$I = \frac{B}{\mu_0 n}$$

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

$$I = \frac{20 \times 10^{-3}}{4\pi \times 10^{-7} \times 2000} = \frac{20 \times 10^{-3}}{8\pi \times 10^{-4}}$$
$$I = \frac{25}{\pi} \approx 7.96\text{ A} \approx 8.0\text{ A}$$
2
A long solenoid is made by closely winding a wire of radius 0.5 mm over a cylindrical nonmagnetic frame so that successive turns nearly touch each other. What will be the magnetic field at the centre of the solenoid if a current of 5 A flows through it?
Answer $2\pi \times 10^{-3}\text{ T}$ 📝
Detailed Solution

Wire radius $r = 0.5\text{ mm}$. Since the turns touch each other, the thickness of one turn equals the diameter of the wire.

$$d = 2r = 2 \times 0.5\text{ mm} = 1.0\text{ mm} = 10^{-3}\text{ m}$$

The number of turns per unit length ($n$) is the reciprocal of the wire diameter:

$$n = \frac{1}{d} = \frac{1}{10^{-3}} = 1000\text{ turns/m}$$

Calculate the magnetic field ($B$) for a current $I = 5\text{ A}$:

$$B = \mu_0 n I = (4\pi \times 10^{-7}) \times 1000 \times 5$$
$$B = 20\pi \times 10^{-4} = 2\pi \times 10^{-3}\text{ T}$$
3
The magnetic field at the centre of a 50 cm long solenoid is $4.0 \times 10^{-2}\text{ T}$ when a current of 8.0 A flows through it. What is the number of turns in the solenoid? Take $\pi=3.14$.
Answer 1990 📝
Detailed Solution

Given parameters: Length $L = 50\text{ cm} = 0.5\text{ m}$, Magnetic field $B = 4.0 \times 10^{-2}\text{ T}$, Current $I = 8.0\text{ A}$.

Using the formula for magnetic field in terms of total turns $N$:

$$B = \frac{\mu_0 N I}{L} \implies N = \frac{B \cdot L}{\mu_0 I}$$

Substitute the given values (using $\pi = 3.14$):

$$N = \frac{4.0 \times 10^{-2} \times 0.5}{4 \times 3.14 \times 10^{-7} \times 8.0} = \frac{0.02}{100.48 \times 10^{-7}}$$
$$N = \frac{200000}{100.48} \approx 1990.45$$

Rounding to the nearest whole turn yields approximately 1990 turns.

4
A solenoid is 1.0 m long and 3.0 cm in diameter. It has five layers of windings of 850 turns each and carries a current of 5.0 A. (i) What is B at its centre? (ii) What is the magnetic flux $\Phi$ for a cross-section of the solenoid at the centre?
Answer (i) $2.67 \times 10^{-2}\text{ T}$, (ii) $1.9 \times 10^{-5}\text{ Wb}$ 📝
Detailed Solution

Length $L = 1.0\text{ m}$, Diameter $= 3.0\text{ cm} \implies$ Radius $r = 1.5\text{ cm} = 0.015\text{ m}$. Current $I = 5.0\text{ A}$.

(i) Calculate magnetic field ($B$):
Total number of turns ($N$) is 5 layers of 850 turns each.

$$N = 5 \times 850 = 4250\text{ turns}$$
$$B = \frac{\mu_0 N I}{L} = \frac{4\pi \times 10^{-7} \times 4250 \times 5.0}{1.0}$$
$$B = 85000\pi \times 10^{-7} \approx 2.67 \times 10^{-2}\text{ T}$$

(ii) Calculate magnetic flux ($\Phi$):
The magnetic flux through the cross-sectional area ($A$) is given by $\Phi = B \cdot A$.

$$A = \pi r^2 = \pi (0.015)^2$$
$$\Phi = (2.67 \times 10^{-2}) \times \pi \times 0.000225 \approx 1.88 \times 10^{-5}\text{ Wb}$$

Rounded to two significant figures: $1.9 \times 10^{-5}\text{ Wb}$.

5
A solenoid is 2.0 m long and 3.0 cm in diameter. It has 5 layers of winding of 1000 turns each and carries a current of 5.0 A. What is the magnetic field at the centre? Use the standard value of $\mu_0$.
Answer $1.57 \times 10^{-2}\text{ T}$ 📝
Detailed Solution

Length $L = 2.0\text{ m}$, Current $I = 5.0\text{ A}$.
Total number of turns $N = 5 \times 1000 = 5000\text{ turns}$.

Calculate the magnetic field ($B$):

$$B = \frac{\mu_0 N I}{L} = \frac{4\pi \times 10^{-7} \times 5000 \times 5.0}{2.0}$$
$$B = \frac{100000\pi \times 10^{-7}}{2} = 50000\pi \times 10^{-7}$$
$$B = 5\pi \times 10^{-3} \approx 5 \times 3.1416 \times 10^{-3}$$
$$B \approx 15.7 \times 10^{-3}\text{ T} = 1.57 \times 10^{-2}\text{ T}$$
6
A toroid has a core of inner radius 20 cm and outer radius 22 cm around which 4200 turns of a wire are wound. If the current in the wire is 10 A, what is the magnetic field (i) inside the core of toroid (ii) outside the toroid and (iii) in the empty space surrounded by the toroid.
Answer (i) 0.04 T (ii) Zero (iii) Zero 📝
Detailed Solution

Number of turns $N = 4200$, Current $I = 10\text{ A}$.
For the core of the toroid, the effective mean radius ($r$) is the average of the inner and outer radii:

$$r = \frac{20 + 22}{2} = 21\text{ cm} = 0.21\text{ m}$$

(i) Inside the core of the toroid:

$$B = \frac{\mu_0 N I}{2\pi r} = \frac{4\pi \times 10^{-7} \times 4200 \times 10}{2\pi \times 0.21}$$
$$B = \frac{2 \times 10^{-7} \times 42000}{0.21} = \frac{0.0084}{0.21} = 0.04\text{ T}$$

(ii) Outside the toroid:
According to Ampere’s Law, an Amperian loop outside the toroid encloses equal and opposite currents (current going in and coming out), making the net enclosed current zero. Thus, $B = 0$.

(iii) In the empty space surrounded by the toroid:
An Amperian loop inside the empty inner space encloses no current ($I_{enclosed} = 0$). Thus, $B = 0$.

7
A long straight solid conductor of radius 4 cm carries a current of 2 A, which is uniformly distributed over its circular cross-section. Find the magnetic field at a distance of 3 cm from the axis of the conductor.
Answer $7.5 \times 10^{-6}\text{ T}$ 📝
Detailed Solution

Radius of conductor $R = 4\text{ cm} = 0.04\text{ m}$. Total current $I = 2\text{ A}$.
We need to find the field at distance $r = 3\text{ cm} = 0.03\text{ m}$. Since $r < R$, the point is inside the conductor.

Using Ampere’s Law for a uniform current distribution, the magnetic field inside a solid cylindrical conductor is proportional to the distance from the axis:

$$B = \frac{\mu_0 I r}{2\pi R^2}$$

Substitute the given values:

$$B = \frac{4\pi \times 10^{-7} \times 2 \times 0.03}{2\pi \times (0.04)^2}$$
$$B = \frac{2 \times 10^{-7} \times 0.06}{0.0016} = \frac{1.2 \times 10^{-8}}{0.0016}$$
$$B = 7.5 \times 10^{-6}\text{ T}$$

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