Problem 1868
Question
The magnetic induction at a point \(P\) which is at a distance \(4 \mathrm{~cm}\) from a long current carrying wire is \(10^{-8}\) tesla. The field of induction at a distance \(12 \mathrm{~cm}\) from the same current would be tesla. (a) \(3.33 \times 10^{-9}\) (b) \(1.11 \times 10^{-4}\) (c) \(3 \times 10^{-3}\) (d) \(9 \times 10^{-2}\)
Step-by-Step Solution
Verified Answer
The magnetic induction at a distance of 12 cm from the same current-carrying wire is \(3.33 \times 10^{-9}\) tesla.
1Step 1: Write down the formula for the magnetic field of a long current-carrying wire
The formula for the magnetic field B produced by a long current-carrying wire is given by:
\[B = \frac{\mu_0 I}{2\pi r}\]
where μ₀ is the permeability of free space, I is the current through the wire, and r is the distance from the wire.
2Step 2: Calculate the magnetic field at 3 times the distance
We need to find the magnetic induction when the distance r is tripled. Let B₁ be the magnetic induction at a distance r and B₂ be the magnetic induction at a distance 3r.
By substituting 3r in place of r, we get:
\[B_2 = \frac{\mu_0 I}{2\pi(3r)}\]
3Step 3: Find the ratio of B₂ to B₁
Now, we will find the ratio of B₂ to B₁:
\[\frac{B_2}{B_1} = \frac{\frac{\mu_0 I}{2\pi(3r)}}{\frac{\mu_0 I}{2\pi r}}\]
4Step 4: Simplify the ratio
Simplify the expression by canceling the common terms in the numerator and denominator:
\[\frac{B_2}{B_1} = \frac{r}{3r} = \frac{1}{3}\]
5Step 5: Find the new magnetic induction
We know that the magnetic induction at a distance r (4 cm) is given as \(10^{-8}\) tesla. Now, we can find the magnetic induction at a distance 3r (12 cm) by multiplying the known induction by the ratio we found in Step 4:
\[B_2 = B_1 \times \frac{1}{3} = (10^{-8}) \times \frac{1}{3}\]
6Step 6: Calculate B₂
Calculate the new magnetic induction:
\[B_2 = 10^{-8} \times \frac{1}{3} = 3.33 \times 10^{-9}\mathrm{~tesla}\]
7Step 7: Choose the correct answer
From our calculations, the magnetic induction at a distance of 12 cm from the same current-carrying wire is \(3.33 \times 10^{-9}\) tesla. Therefore, the correct answer is:
(a) \(3.33 \times 10^{-9}\)
Key Concepts
Magnetic InductionAmpere's LawPermeability of Free Space
Magnetic Induction
Magnetic induction is simply a way to measure the strength of a magnetic field at a specific point in space. It tells us how much magnetic influence is present around an object. This measurement is particularly useful for understanding how magnetic forces might affect nearby objects, like a compass needle or electronic circuits.
The formula for finding magnetic induction produced by a long, straight wire carrying a current (I) is:
The formula for finding magnetic induction produced by a long, straight wire carrying a current (I) is:
- \[B = \frac{\mu_0 I}{2\pi r}\]
Ampere's Law
Ampere's Law is an essential principle in magnetism, providing a straightforward way to determine the magnetic field generated by a current-carrying conductor. It states that the line integral of the magnetic field \(B\) along a closed path is proportional to the current \(I\) that passes through the enclosed area. In mathematical terms, Ampere's Law is represented by:
For straight wires like in our exercise problem, Ampere's Law assists in deriving the magnetic field formula used. The law simplifies to finding the magnetic field at a point along a path around a current, leading to the direct formula:
- \[\oint B \cdot dl = \mu_0 I\]
For straight wires like in our exercise problem, Ampere's Law assists in deriving the magnetic field formula used. The law simplifies to finding the magnetic field at a point along a path around a current, leading to the direct formula:
- \[B = \frac{\mu_0 I}{2\pi r}\]
Permeability of Free Space
Permeability of free space, denoted by \(\mu_0\), represents the ability of a vacuum to support the presence of a magnetic field. It is a fundamental physical constant with a value of approximately \(4\pi \times 10^{-7} \mathrm{~Tm/A}\). This term appears in many formulas relating to magnetic fields and circuits, signifying how vacuum as a medium responds to magnetic influences.
In the magnetic field formula used for our exercise, \(\mu_0\) is crucial:
Understanding \(\mu_0\) helps grasp the concept of magnetic fields in environments devoid of material stirring resistance, giving a foundation for calculating fields in much more complex settings.
In the magnetic field formula used for our exercise, \(\mu_0\) is crucial:
- \[B = \frac{\mu_0 I}{2\pi r}\]
Understanding \(\mu_0\) helps grasp the concept of magnetic fields in environments devoid of material stirring resistance, giving a foundation for calculating fields in much more complex settings.
Other exercises in this chapter
Problem 1862
Two straight long conductors \(\mathrm{AOB}\) and \(\mathrm{COD}\) are perpendicular to each other and carry currents \(\mathrm{I}_{1}\) and \(\mathrm{I}_{2}\).
View solution Problem 1867
If a long hollow copper pipe carries a direct current, the magnetic field associated with the current will be (a) Only inside the pipe (b) Only outside the pipe
View solution Problem 1869
The strength of the magnetic field at a point \(\mathrm{y}\) near a long straight current carrying wire is \(\mathrm{B}\). The field at a distance \(\mathrm{y}
View solution Problem 1870
The mag. field (B) at the centre of a circular coil of radius "a", through which a current I flows is (a) \(\mathrm{B} \propto \mathrm{c} \mathrm{a}\) (b) \(\ma
View solution