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Earth's Moment The magnitude of magnetic dipole moment of Earth is \(8.00 \times 10^{22} \mathrm{~J} / \mathrm{T}\). Assume that this is produced by charges flowing in Earth's molten outer core. If the radius of their circular path is \(3500 \mathrm{~km}\), calculate the amount of current associated with each moving charge.

Short Answer

Expert verified
The current is approximately \( 2.08 \times 10^9 \text{ A} \).

Step by step solution

01

Identify the given values

The magnetic dipole moment, \( M \), is given as \( 8.00 \times 10^{22} \text{ J/T} \) and the radius, \( r \), of the circular path is given as \( 3500 \text{ km} = 3.5 \times 10^6 \text{ m} \).
02

Understand the relationship

The magnetic dipole moment, \( M \), for a current loop is given by the formula \( M = I \times A \), where \( I \) is the current and \( A \) is the area of the loop.
03

Calculate the area of the loop

The area \( A \) of a circle is given by \( A = \pi r^2 \). Substituting the given radius, \( A = \pi \times (3.5 \times 10^6 \text{ m})^2 \).
04

Compute the area

Evaluate \( A = \pi \times (3.5 \times 10^6 \text{ m})^2 = \pi \times 12.25 \times 10^{12} \text{ m}^2 = 38.48 \times 10^{12} \text{ m}^2 = 3.848 \times 10^{13} \text{ m}^2 \).
05

Solve for the current

Using \( M = I \times A \), substitute the values to find \( I \). So, \( I = \frac{M}{A} = \frac{8.00 \times 10^{22} \text{ J/T}}{3.848 \times 10^{13} \text{ m}^2} \).
06

Compute the current

Calculate \( I = \frac{8.00 \times 10^{22} \text{ J/T}}{3.848 \times 10^{13} \text{ m}^2} = 2.08 \times 10^9 \text{ A} \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Earth's magnetic field
The Earth functions like a gigantic magnet. This is due to electric currents generated in its molten outer core. These currents create a magnetic dipole moment, which is a way to measure the Earth's magnetism. The magnetic dipole moment of Earth is substantial, estimated at around \(8.00 \times 10^{22}\) J/T (Joules per Tesla). A helpful analogy is to think about small magnets or compass needles that align themselves along the Earth's magnetic field lines. This magnetic field not only impacts compasses but also plays a crucial role in shielding our planet from harmful solar wind particles. The area in which the magnetic forces are effective, extending well beyond the atmosphere, is known as the magnetosphere.
Current calculation
When we try to calculate the current creating this magnetic field, we rely on the concept of a current loop. Picture a circular loop with a known radius where the current travels. The relationship between the magnetic dipole moment, current, and the area of the loop is simplified using the formula \(M = I \times A\). Here, \(M\) stands for the magnetic dipole moment, \(I\) is the current, and \(A\) is the area of the loop.
Magnetic moment computation
To compute the current, we also need to understand how to calculate the area of the loop (\(A\)). Given the radius of the circular path, which for Earth’s core is \(3500\) km (\(3.5 \times 10^6\) meters), the area can be calculated using the formula \(A = \text{π} r^2\). This gives \(A = \text{π} \times (3.5 \times 10^6 \text{ m})^2 = 3.848 \times 10^{13} \text{ m}^2\). Using the formula \(I = \frac{M}{A}\), we can substitute \(M = 8.00 \times 10^{22}\) J/T and \(A = 3.848 \times 10^{13}\) m² to get \(I = \frac{8.00 \times 10^{22}}{3.848 \times 10^{13}} = 2.08 \times 10^9\) A (Amperes). This result shows that a significant amount of current is responsible for generating Earth's magnetic field.

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Most popular questions from this chapter

ABCDEFA Figure \(\quad 29-36\) \(\begin{array}{l}\text { shows } a & \text { current } \text { loop }\end{array}\) \(A B C D E F A\) carrying a current \(i\) \(=5.00 \mathrm{~A}\). The sides of the loop are parallel to the coordinate axes, with \(A B=20.0 \mathrm{~cm}, B C=\) \(30.0 \mathrm{~cm}\), and \(F A=10.0 \mathrm{~cm}\). Calculate the magnitude and direction of the magnetic dipole moment of this loop. (Hint: Imagine equal and opposite currents \(i\) in the line segment \(A D\); then treat the two rectangular loops \(A B C D A\) and \(A D E F A .)\)

Copper Rod A \(1.0 \mathrm{~kg}\) copper rod rests on two horizontal rails \(1.0 \mathrm{~m}\) apart and carries a current of \(50 \mathrm{~A}\) from one rail to the other. The coefficient of static friction between rod and rails is \(0.60 .\) What is the magnitude of the smallest magnetic field (not necessarily vertical) that would cause the rod to slide?

Heavy Ions Physicist S. A. Goudsmit devised a method for measuring the masses of heavy ions by timing their periods of revolution in a known magnetic field. A singly charged ion of iodine makes \(7.00\) rev in a field of \(45.0 \mathrm{mT}\) in \(1.29 \mathrm{~ms}\). Calculate its mass, in atomic mass units. (Actually, the method allows mass measurements to be carried out to much greater accuracy than these approximate data suggest.)

A Velocity Selector A group of physicists at Argonne National Laboratory in Illinois wants to bombard metals with monoenergetic beams of alpha particles to study radiation damage. (Alpha particles are helium nuclei, which consist of two neutrons and two protons and thus have a net charge of \(+2 e\) where \(e\) is the amount of the charge on the electron.) They have managed to create a beam of alpha particles from the decay of radioactive elements, but some of the alpha particles lose energy as they collide with other atoms in the source. As a new physicist assigned to the group you have been asked to use a velocity selector to select only the alpha particles in the beam that are close to one velocity and get rid of the others. The velocity selector consists of: (1) a power supply capable of de- livering large potential differences between capacitor plates and (2) a large permanent magnet that has a uniform magnetic field perpendicular to the beam. The setup for the velocity selector is shown in Fig. 29-38. The direction of the \(\mathrm{B}\) -field is out of the paper. Your magnet has a field of \(0.22 \mathrm{~T}\) and the capacitor plates have a spacing of \(2.5 \mathrm{~cm}\). You are asked to figure out how the velocity selector works and then tell your group what voltage to put across the capacitor plates to select a velocity of \(4.2 \times 10^{6} \mathrm{~m} / \mathrm{s} .\) This is your first job and you feel overwhelmed by the assignment, but you calm down and begin to analyze the situation one step at a time. You come up with the following: (a) The magnet is oriented so its magnetic field is out of the paper in the diagram you are given, so you use the right-hand rule to determine the direction of the magnetic force on an alpha particle passing from left to right into the magnetic field. What direction did you come up with for the force? (b) You realize that by using \(\vec{F}^{\prime} \mathrm{mag}=q \vec{v} \times \vec{B}\), you can calculate the magnitude of force on an alpha particle moving at speed \(v\) just as it enters the uniform magnetic field as a function of the charge on the alpha particle and the magnitude of the magnetic field \(B\). What is the expression for the magnitude of the force in terms of \(e\), \(v\), and \(B ?\) (c) You realize that you might be able to put just the right voltage across the two capacitor plates so that the electrical force on a given alpha particle will be equal in magnitude and opposite in direction to the Lorentz magnetic force. Then any alpha particles with just the right velocity will pass straight through the poles of the magnet without being deflected. First you think about whether the voltage on the upper capacitor plate should be positive or negative to give a canceling force. What do you decide? (d) Next you realize that if you know the electric field between the plates and the charge on the alpha particle then you can compute the electrical force on it. What is the relationship between the electrical force \(\vec{F}^{\text {elec }}\), charge, \(q\), and electric field \(\vec{E} ?\) (e) Finally, you use the fact that the magnitude of the electric field between capacitor plates is given by \(E=|\Delta V| / d\) where \(d\) is the spacing between the plates. Show that the voltage needed to have the electrical force and the magnetic force be "equal and opposite" can be calculated using the equation \(|\Delta V|=v B d\). Calculate the voltage needed.

Field Perpendicular to Beam A uniform magnetic field is applied perpendicular to a beam of electrons moving at \(1.3 \times 10^{6} \mathrm{~m} / \mathrm{s}\). What is the magnitude of the field if the electrons travel in a circular arc of radius \(0.35 \mathrm{~m}\) ?

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