Problem 9
Question
The magnetic field normal to the plane of a wire of \(n\) turns and radius \(r\) which carries a current \(i\) is measured on the axis of the coil at a small distance \(h\) from the centre of the coil. This is smaller than the magnetic field at the centre by the fraction (a) \((2 / 3) r^{2} / h^{2}\) (b) \((3 / 2) r^{2} / h^{2}\) (c) \((2 / 3) h^{2} / r^{2}\) (d) \((3 / 2) h^{2} / r^{2}\)
Step-by-Step Solution
Verified Answer
The correct answer is (d) \(\frac{3}{2} \frac{h^2}{r^2}\).
1Step 1: Understand the Magnetic Field at the Center
The magnetic field at the center of a circular coil with radius \( r \) and \( n \) turns carrying current \( i \) is given by the formula \( B_{center} = \frac{\mu_0 n i}{2r} \), where \( \mu_0 \) is the permeability of free space.
2Step 2: Calculate Magnetic Field on the Axis
The magnetic field at a point on the axis at a distance \( h \) from the center of the coil is given by \( B_{axis} = \frac{\mu_0 n i r^2}{2(r^2 + h^2)^{3/2}} \).
3Step 3: Calculate the Difference in Magnetic Field
To find the fractional smaller field, note that \( B_{center} - B_{axis} \) needs to be expressed as a fraction of \( B_{center} \). This fraction is what the question asks to determine.
4Step 4: Set up the Fraction of the Difference
The fractional difference is \( \frac{B_{center} - B_{axis}}{B_{center}} = 1 - \frac{2r}{\sqrt{(r^2 + h^2)^3}} \approx \frac{3}{2} \cdot \frac{h^2}{r^2} \) for small \( h/r \).
5Step 5: Use Approximation for Small Distances
Assume \( h << r \), then \( (r^2 + h^2)^{3/2} \approx r^3 \left(1 + \frac{3h^2}{2r^2}\right) \) and simplify the expression.
6Step 6: Compare with Given Options
Compare the derived expression \( \frac{3}{2} \frac{h^2}{r^2} \) to the given options: (a) \( \frac{2}{3} \frac{r^2}{h^2} \), (b) \( \frac{3}{2} \frac{r^2}{h^2} \), (c) \( \frac{2}{3} \frac{h^2}{r^2} \), (d) \( \frac{3}{2} \frac{h^2}{r^2} \).
7Step 7: Identify the Correct Option
The fraction \( \frac{3}{2} \frac{h^2}{r^2} \) exactly matches option (d), therefore, this is the correct answer.
Key Concepts
Circular Coil Magnetic FieldMagnetic Field Axis FormulaMagnetic Field Calculation
Circular Coil Magnetic Field
The magnetic field within a circular coil is an essential concept in electromagnetism. Let's explore how it works. A circular coil comprises a wire wound in loops or turns, and when current flows through these turns, a magnetic field is created. The principle at play here is that any current-carrying conductor generates a magnetic field around it.
In the case of a circular coil with a certain number of turns, denoted by \( n \), the magnetic field at the center of this coil is intensified due to the cumulative effect of each loop or turn. This magnetic field can be quantified using the formula:
In the case of a circular coil with a certain number of turns, denoted by \( n \), the magnetic field at the center of this coil is intensified due to the cumulative effect of each loop or turn. This magnetic field can be quantified using the formula:
- \( B_{center} = \frac{\mu_0 n i}{2r} \)
- \( \mu_0 \) is the permeability of free space, a constant \( 4\pi \times 10^{-7} \ \text{Tm/A} \)
- \( n \) is the number of turns
- \( i \) is the current
- \( r \) is the radius of the coil
Magnetic Field Axis Formula
The magnetic field also exists along the axis of the circular coil, but it varies depending on the distance from the center. If you measure the field at a point along this axis, at a distance \( h \) from the center, the field strength changes. This alteration is captured by the magnetic field axis formula, expressed as:
- \( B_{axis} = \frac{\mu_0 n i r^2}{2(r^2 + h^2)^{3/2}} \)
- The distance \( h \) from the coil's center
- How the radius and the distance combine to affect the field strength. The term \((r^2 + h^2)^{3/2}\) reflects the geometrical relationship between different distances.
Magnetic Field Calculation
Once you understand how the magnetic field varies from the center to the axis, it becomes possible to calculate and compare these differences. The key question in exercises like these is to determine how the axis field compares to the center field. To solve this, we find the fractional difference:
- Fractional difference: \( \frac{B_{center} - B_{axis}}{B_{center}} \)
- \( 1 - \frac{2r}{\sqrt{(r^2 + h^2)^3}} \approx \frac{3}{2} \cdot \frac{h^2}{r^2} \)
Other exercises in this chapter
Problem 7
Two long and parallel straight wires \(A\) and \(B\) carrying currents of \(8.0 \mathrm{~A}\) and \(5.0 \mathrm{~A}\) in the same direction are separated by a d
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A length \(l\) of wire carries a steady current \(i\). It is bent first to form a circular plane coil of one turn. The same length is now bent more sharply to g
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The magnetic field of the earth can be modelled by that of a point dipole placed at the centre of the earth. The dipole axis makes an angle of \(11.3^{\circ}\)
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A pulsar is a neutron star having magnetic field at \(10^{12} \mathrm{G}\) at its surface. The maximum magnetic force experienced by an electron moving with vel
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