Problem 1968
Question
A small bar magnet has a magnetic moment \(1.2 \mathrm{~A} \cdot \mathrm{m}^{2}\). The magnetic field at a distance \(0.1 \mathrm{~m}\) on its axis will be tesla. (a) \(1.2 \times 10^{-4}\) (b) \(2.4 \times 10^{-4}\) (c) \(2.4 \times 10^{4}\) (d) \(1.2 \times 10^{4}\)
Step-by-Step Solution
Verified Answer
The magnetic field at a distance of \(0.1\,\mathrm{m}\) along the axis of the given small bar magnet is \(2.4 \times 10^{-4} \mathrm{T}\). Answer: (b) \(2.4 \times 10^{-4}\).
1Step 1: Recall the formula for magnetic field due to a magnetic dipole
The magnetic field B due to a magnetic dipole at a point on its axis is given by the formula: \[B = \frac{\mu_0}{4\pi} \cdot \frac{2M}{r^3}\]
Where \(B\) is the magnetic field, \(\mu_0\) is the permeability of free space (equal to \(4\pi \times 10^{-7} \mathrm{T} \cdot \mathrm{m} / \mathrm{A}\)), \(M\) is the magnetic moment, and \(r\) is the distance from the dipole along its axis.
2Step 2: Substitute the given values into the formula
Given values are \(M = 1.2 \,\mathrm{A} \cdot \mathrm{m}^2\) and \(r = 0.1\,\mathrm{m}\). Substitute these values into the formula for the magnetic field:
\[B =\frac{\mu_0}{4\pi} \cdot \frac{2(1.2\,\mathrm{A} \cdot \mathrm{m}^2)}{(0.1\,\mathrm{m})^3}\]
3Step 3: Calculate the magnetic field
Using \(\mu_0 = 4\pi \times 10^{-7} \mathrm{T} \cdot \mathrm{m} / \mathrm{A}\), let's plug in the value and calculate the magnetic field:
\[B = \frac{(4\pi \times 10^{-7} \mathrm{T} \cdot \mathrm{m} / \mathrm{A})}{4\pi} \cdot \frac{2(1.2\,\mathrm{A} \cdot \mathrm{m}^2)}{(0.1\,\mathrm{m})^3}\]
Simplify the expression:
\[B = 10^{-7} \mathrm{T} \cdot \mathrm{m} / \mathrm{A} \cdot \frac{2.4\,\mathrm{A} \cdot \mathrm{m}^2}{0.001\,\mathrm{m}^3}\]
\[B = 2.4 \times 10^{-4} \mathrm{T}\]
4Step 4: Match the calculated value with the given options
We find that the magnetic field at a distance of \(0.1\,\mathrm{m}\) along the axis of the given small bar magnet is \(2.4 \times 10^{-4} \mathrm{T}\), which corresponds to option (b).
Answer: (b) \(2.4 \times 10^{-4}\)
Key Concepts
Magnetic MomentMagnetic Dipole FormulaPermeability of Free Space
Magnetic Moment
In the context of magnetism, the magnetic moment is a vector quantity that measures the strength and direction of a magnetic source's magnetism. It represents the extent to which the magnetic source can produce a magnetic field and interact with external magnetic fields. The magnetic moment (M) is usually expressed in units of amperes per square meter (\( ext{A} \, ext{m}^2 \)). A higher magnetic moment indicates a stronger capability to produce a magnetic effect. For example, in our exercise, a bar magnet has a magnetic moment of \( 1.2 \, ext{A} \, ext{m}^2 \), signifying its strength relative to other magnets. This property is essential as it directly influences the strength of the magnetic field a magnet can create at a certain distance.
Magnetic Dipole Formula
The magnetic dipole formula calculates the magnetic field produced by a magnetic dipole, especially at a point on its axis. The formula is expressed as: \[ B = \frac{\mu_0}{4\pi} \cdot \frac{2M}{r^3} \]Here:
- \( B \) is the magnetic field.
- \( \mu_0 \) is the permeability of free space.
- \( M \) is the magnetic moment.
- \( r \) is the distance from the dipole.
Permeability of Free Space
The permeability of free space, also called the magnetic constant, is a fundamental physical constant used in magnetism calculations. It is denoted by \( \mu_0 \) and defined as \( 4\pi \times 10^{-7} \, \text{T} \cdot \text{m} / \text{A} \).This constant essentially quantifies the extent to which a magnetic field can penetrate the classical vacuum, i.e., space devoid of matter.In the magnetic dipole formula, \( \mu_0 \) plays a crucial role in determining the ultimate value of the magnetic field created by a dipole. Its presence is necessary to convert the units appropriately and achieve the correct formula form.Understanding \( \mu_0 \) is vital as it forms the basis for how magnetic fields operate in free space, providing insight into magnetic force and interactions.
Other exercises in this chapter
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