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A solid cylinder carries a current that is uniform over its cross section. Where is the magnitude of the magnetic field the greatest? a) at the center of the cylinder's cross section b) in the middle of the cylinder c) at the surface d) none of the above

Short Answer

Expert verified
Answer: c) at the surface

Step by step solution

01

Ampère's Law

Ampère's Law states that the integral of the magnetic field B around a closed loop (or Amperian loop) is equal to the product of the permeability of free space (μ₀) and the total current passing through the loop. Mathematically, it is expressed as: ∮B⃗ · d⃗l = μ₀ * I_enclosed In cylindrical coordinates, the magnetic field generated by the current in the cylinder will have only the azimuthal component.
02

Consider points inside the cylinder

We need to evaluate the magnetic field inside the cylinder at a radial distance r from the central axis where 0 ≤ r ≤ R, with R being the radius of the cylinder. The field inside the cylinder depends on the portion of the current enclosed inside the Amperian loop. The Amperian loop will be a circle with radius r inside the cylinder. We need to find the enclosed current inside this loop. Let the current per unit area be J (in A/m²). Then, the total current flowing through the cylinder can be found by integrating J over the cylinder's cross-sectional area. The enclosed current within the Amperian loop is: I_enclosed = J * π * r²
03

Use Ampère's Law for points inside the cylinder

Now, using Ampère's Law for points inside the cylinder: ∮B⃗ · d⃗l = B * 2 * π * r = μ₀ * J * π * r² Solving for B, we have: B_inside = (μ₀ * J * r) / 2
04

Consider points outside the cylinder

For points outside the cylinder (i.e., r > R), the entire current is enclosed within the Amperian loop. The current enclosed is then: I_enclosed = J * π * R²
05

Use Ampère's Law for points outside the cylinder

Using Ampère's Law for points outside the cylinder: ∮B⃗ · d⃗l = B * 2 * π * r = μ₀ * J * π * R² Solving for B, we have: B_outside = (μ₀ * J * R²) / (2 * r)
06

Compare the magnetic field magnitudes

Now we can compare the magnetic field's magnitudes depending on the radial distance r: - At the center of the cylinder's cross section (r = 0), the magnetic field B_inside = 0. - In the middle of the cylinder (0 < r < R), the magnetic field B_inside is proportional to r. - At the surface (r = R), B_outside = (μ₀ * J * R) / 2. - For points outside the cylinder (r > R), the magnetic field B_outside decreases with increasing r.
07

Determine the location of the greatest magnitude

Based on the comparison, we can see that as we move from the center to the surface, the magnetic field's magnitude increases from 0 to a maximum value (μ₀ * J * R) / 2 at the surface, and then decreases as we move further away from the surface. Therefore, the magnitude of the magnetic field is the greatest at the surface of the cylinder. The correct answer is: c) at the surface

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Most popular questions from this chapter

A \(0.90-\mathrm{m}\) -long solenoid has a radius of \(5.0 \mathrm{~mm}\). When the wire carries a \(0.20-\mathrm{A}\) current, the magnetic field inside the solenoid is \(5.0 \mathrm{mT}\). How manv turns of wire are there in the solenoid?

When a magnetic dipole is placed in a magnetic field, it has a natural tendency to minimize its potential energy by aligning itself with the field. If there is sufficient thermal energy present, however, the dipole may rotate so that it is no longer aligned with the field. Using \(k_{\mathrm{B}} T\) as a measure of the thermal energy, where \(k_{B}\) is Boltzmann's constant and \(T\) is the temperature in kelvins, determine the temperature at which there is sufficient thermal energy to rotate the magnetic dipole associated with a hydrogen atom from an orientation parallel to an applied magnetic field to one that is antiparallel to the applied field. Assume that the strength of the field is \(0.15 \mathrm{~T}\).

Consider two parallel current-carrying wires. The magnetic fields cause attractive forces between the wires, so it appears that the magnetic field due to one wire is doing work on the other wire. How is this explained? a) The magnetic force can do no work on isolated charges; this says nothing about the work it can do on charges confined in a conductor b) Since only an electric field can do work on charges, it is actually the electric fields doing the work here. c) This apparent work is due to another type of force.

A 50 -turn rectangular coil of wire with dimensions \(10.0 \mathrm{~cm}\) by \(20.0 \mathrm{~cm}\) lies in a horizontal plane, as shown in the figure. The axis of rotation of the coil is aligned north and south. It carries a current \(i=1.00 \mathrm{~A}\) and is in a magnetic field pointing from west to east. A mass of \(50.0 \mathrm{~g}\) hangs from one side of the coil. Determine the strength the magnetic field has to have to keep the coil in the horizontal orientation.

A square box with sides of length \(1.00 \mathrm{~m}\) has one corner at the origin of a coordinate system, as shown in the figure. Two coils are attached to the outside of the box. One coil is on the box face that is in the \(x z\) -plane at \(y=0\), and the second is on the box face in the \(y z\) -plane at \(x=1.00 \mathrm{~m} .\) Each of the coils has a diameter of \(1.00 \mathrm{~m}\) and contains 30.0 turns of wire carrying a current of \(5.00 \mathrm{~A}\) in each turn. The current in each coil is clockwise when the coil is viewed from outside the box. What are the magnitude and the direction of the magnetic field at the center of the box?

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