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Having just learned that there is energy associated with magnetic fields, an inventor sets out to tap the energy associated with the Earth's magnetic field. What volume of space near Earth's surface contains 1.00 J of energy, assuming the strength of the magnetic field to be \(5.00 \cdot 10^{-5} \mathrm{~T} ?\)

Short Answer

Expert verified
Answer: The volume of space near the Earth's surface that contains 1 Joule of energy is approximately 1.005 x 10^9 m^3.

Step by step solution

01

Recall the formula for magnetic field energy density

The energy density of a magnetic field is given by the formula: \(u = \frac{1}{2} \frac{B^{2}}{\mu_0}\) Where \(u\) is the energy density, \(B\) is the magnetic field strength, and \(\mu_0 = 4 \pi \cdot 10^{-7} \mathrm{~ T m/A}\) is the permeability of free space.
02

Calculate the energy density

Using the given magnetic field strength \(B = 5.00 \cdot 10^{-5} \mathrm{~T}\), we can calculate the energy density \(u\): \( u = \frac{1}{2} \frac{(5.00 \cdot 10^{-5} \text T)^2}{4 \pi \cdot 10^{-7} \text T \cdot \text m/\text A}\) Calculate the energy density: \(u = 9.95 \cdot 10^{-10} \mathrm{ \frac{J}{m^3}}\)
03

Calculate the required volume

Now we can find the volume \(V\) that contains 1 Joule of magnetic field energy by dividing the total energy by the energy density: \(V = \frac{E}{u}\) Where \(E = 1.00 \text J\) (given) and \(u\) is the energy density calculated in step 2. Plug in the values: \(V = \frac{1.00 \text J}{9.95 \cdot 10^{-10} \frac{\text J}{\text m^{3}}}\) Calculate the volume: \(V = 1.005 \cdot 10^9 \text m^{3}\) So, the volume of space near Earth's surface that contains 1 Joule of energy is approximately \(1.005 \cdot 10^9 \mathrm{~m^3}\).

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Key Concepts

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

Energy Density
Energy density is a fundamental concept in physics, especially when dealing with fields such as electromagnetism. It refers to the amount of energy stored in a given system or region of space per unit volume. For magnetic fields, this is crucial to understanding many aspects of their behavior and potential for work. In the context of our exercise, the energy density tells us how much energy is contained within a specific volume of the magnetic field.

The formula to calculate the magnetic field's energy density, \( u = \frac{1}{2} \frac{B^{2}}{\mu_0} \), is derived from the work required to establish the magnetic field within a vacuum. Here, \( B \) represents the magnetic field strength, and \( \mu_0 \) is the permeability of free space. When we substitute the Earth's magnetic field into this formula, we can determine the energy per cubic meter, which is important for applications like the inventor's quest to tap into this energy.
Permeability of Free Space
The permeability of free space, denoted by \( \mu_0 \), is a physical constant that is essential to the study of electromagnetism. It represents the extent to which a magnetic field can permeate a vacuum, which is the 'space' free of any material or substance. In simpler terms, it's a measure of how easy it is for a magnetic field to spread out in empty space.

The value of \( \mu_0 \) is \( 4 \pi \cdot 10^{-7} \text T m/A \), which arises naturally in the equations of electromagnetism, and also relates electric and magnetic units in the International System of Units (SI). When calculating the energy density of a magnetic field, as was demonstrated in our exercise, the permeability of free space has to be factored in to account for the natural 'resistance' that space offers to magnetic forces. Understanding this constant is vital for engineers and scientists as they design systems and tools that interface with magnetic fields.
Magnetic Field Strength
Magnetic field strength, symbolized by \( B \), is one of the most significant characteristics of a magnetic field. It describes the force that a magnetic field exerts on moving electric charges and magnetic materials, commonly measured in teslas (T) in the International System of Units (SI). A higher magnetic field strength means a stronger ability to affect the surrounding environment.

In the given exercise, the Earth's magnetic field strength is quoted as \( 5.00 \cdot 10^{-5} \text T \), which is typical for the Earth's surface. Magnetic field strength is especially relevant in technology and physical sciences, influencing everything from electric motors to the behavior of charged particles in space. The inventor who aims to exploit the Earth's magnetic field will rely on accurately gauging its strength to estimate the potential energy that could be harnessed for practical uses.

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Most popular questions from this chapter

A long solenoid with a circular cross section of radius \(r_{1}=2.80 \mathrm{~cm}\) and \(n=290\) turns/cm is inside of and coaxial with a short coil that has a circular cross section of radius \(r_{2}=4.90 \mathrm{~cm}\) and \(N=31\) turns. Suppose the current in the short coil is increased steadily from zero to \(i=2.80 \mathrm{~A}\) in \(18.0 \mathrm{~ms} .\) What is the magnitude of the potential difference induced in the solenoid while the current in the short coil is changing? a) \(0.0991 \mathrm{~V}\) b) \(0.128 \mathrm{~V}\) c) \(0.233 \mathrm{~V}\) d) \(0.433 \mathrm{~V}\) e) \(0.750 \mathrm{~V}\)

Chapter 14 discussed damped harmonic oscillators, in which the damping force is velocity dependent and always opposes the motion of the oscillator. One way of producing this type of force is to use a piece of metal, such as aluminum, that moves through a nonuniform magnetic field. Explain why this technique is capable of producing a damping force.

A 100 -turn solenoid of length \(8.00 \mathrm{~cm}\) and radius \(6.00 \mathrm{~mm}\) carries a current of 0.400 A from right to left. The current is then reversed so that it flows from left to right. By how much does the energy stored in the magnetic field inside the solenoid change?

A rectangular conducting loop with dimensions \(a\) and \(b\) and resistance \(R\) is placed in the \(x y\) -plane. A magnetic field of magnitude \(B\) passes through the loop. The magnetic field is in the positive \(z\) -direction and varies in time according to \(B=B_{0}\left(1+c_{1} t^{3}\right),\) where \(c_{1}\) is a constant with units of \(1 / \mathrm{s}^{3}\). What is the direction of the current induced in the loop, and what is its value at \(t=1 \mathrm{~s}\) (in terms of \(a, b, R, B_{0},\) and \(\left.c_{1}\right) ?\)

A circular coil of wire with 20 turns and a radius of \(40.0 \mathrm{~cm}\) is laying flat on a horizontal tabletop as shown in the figure. There is a uniform magnetic field extending over the entire table with a magnitude of \(5.00 \mathrm{~T}\) and directed to the north and downward, making an angle of \(25.8^{\circ}\) with the horizontal. What is the magnitude of the magnetic flux through the coil?

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