A straight wire with a constant current running through it is in Earth's magnetic field, at a location where the magnitude is \(0.43 \mathrm{G}\). What is the minimum current that must flow through the wire for a 10.0 -cm length of it to experience a force of \(1.0 \mathrm{~N} ?\)

Short Answer

Expert verified
Answer: The minimum current required is 2.33 x 10^4 A.

Step by step solution

01

Write down the given information and formula

The given information is: - Length of the wire section (L): \(10.0 \, \mathrm{cm} = 0.1 \, \mathrm{m}\) - Earth's magnetic field (B): \(0.43\, \mathrm{G} = 0.43 \times 10^{-4} \, \mathrm{T}\) - Force (F): \(1.0\, \mathrm{N}\) The formula for the magnetic force on the wire is: \(F = I * L * B * \sin(\theta)\)
02

Determine the angle between the current and magnetic field

Since we need the minimum current, the angle between the current and the magnetic field should be such that the magnetic force is maximized. The function \(\sin(\theta)\) is maximized when \(\theta = 90 ^\circ\). So, we have: \(\theta = 90 ^\circ\)
03

Substitute values into the formula and solve for current

Now we will substitute the given values and the angle into the magnetic force formula to find the minimum current (I): \(1.0\, \mathrm{N} = I * 0.1\, \mathrm{m} * (0.43 \times 10^{-4}\, \mathrm{T}) * \sin(90 ^\circ)\) Since \(\sin(90^\circ) = 1\), the equation simplifies to: \(1.0\, \mathrm{N} = I * 0.1\, \mathrm{m} * (0.43 \times 10^{-4}\, \mathrm{T})\) Now, we can solve for the current (I): \(I = \frac{1.0\, \mathrm{N}}{0.1\, \mathrm{m} * (0.43 \times 10^{-4}\, \mathrm{T})} = \frac{1.0}{0.1 * 0.43 \times 10^{-4}}\, \mathrm{A}\) \(I = 2.33 \times 10^4\, \mathrm{A}\) Therefore, the minimum current required for the 10 cm section of the wire to experience a force of \(1.0\, \mathrm{N}\) is \(2.33 \times 10^4\, \mathrm{A}\).

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Key Concepts

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

Lorentz Force
The Lorentz force is a fundamental principle explaining how a magnetic field interacts with electric charges in motion. It refers to the force experienced by a charged particle or, by extension, a current-carrying wire, when it's in the presence of magnetic and electric fields. The formula for the Lorentz force on a wire is expressed as (F = I * L * B * \(sin(\theta)\)), where F is the magnetic force, I is the current, L is the length of the wire, B is the magnetic field strength, and \(\theta\) is the angle between the direction of the current and the magnetic field.

In the context of the exercise provided, the Lorentz force calculates the interaction between Earth's magnetic field and the electrical current running through a wire. Understanding this concept allows us to determine the energy and direction of the force acting on the wire, and by manipulating variables like the current, we can alter the magnitude of this force.
Earth's Magnetic Field
Earth's magnetic field, emanating largely from its core, is a protective and dynamic force that extends far out into space. While this field is most commonly recognized for its role in guiding compasses, it also has critical implications for many scientific and technological applications, including the scenario described in our exercise.

The strength of Earth's magnetic field at the surface typically ranges between about 0.25 to 0.65 Gauss, with variations depending on location and altitude. In the exercise, the wire is situated in a part of Earth's magnetic field that has a strength of 0.43 Gauss. It's important to note that the magnetic field is usually described in Tesla (T) in the SI unit system, and since 1 Gauss is equivalent to \(10^{-4}\) Tesla, students need to convert this measure appropriately to apply the Lorentz force equation.
Current and Magnetic Field Relationship
Understanding the relationship between current and magnetic field is vital in electromagnetism. The direction of the magnetic force on a current-carrying wire is perpendicular both to the direction of the magnetic field and to the current itself, as stated by the right-hand rule. This three-dimensional relationship is encapsulated in the Lorentz force equation mentioned earlier.

The magnitude of the force is directly proportional to the current, length of the wire, magnetic field strength, and the sine of the angle between the wire and the magnetic field (\(sin(\theta)\)). For the maximum force to be experienced, this angle must be 90 degrees, making the sine function equal to 1. This relationship is crucial when solving for the unknown current in the exercise, as we assume the ideal condition where this angle is 90 degrees to calculate the minimum current required to achieve a certain force.
Magnetic Field Strength
Magnetic field strength indicates the intensity of a magnetic field at a given point and is a key factor in determining the force exerted on a moving charged particle or current-carrying conductor. It's denoted by the symbol B and measured in Teslas (T) in the International System of Units (SI). Higher magnetic field strength results in a greater force when all other factors in the Lorentz force equation remain constant.

In the provided exercise, the wire's interaction with Earth's magnetic field is quantified to demonstrate the direct correlation between the magnetic field strength and the force experienced by the wire. If all other conditions remain the same, a stronger magnetic field would mean a greater force on the wire for any given amount of current.

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Most popular questions from this chapter

A coil consists of 120 circular loops of wire of radius \(4.8 \mathrm{~cm} .\) A current of 0.49 A runs through the coil, which is oriented vertically and is free to rotate about a vertical axis (parallel to the \(z\) -axis). It experiences a uniform horizontal magnetic field in the positive \(x\) -direction. When the coil is oriented parallel to the \(x\) -axis, a force of \(1.2 \mathrm{~N}\) applied to the edge of the coil in the positive \(y\) -direction can keep it from rotating. Calculate the strength of the magnetic field.

A circular coil with a radius of \(10.0 \mathrm{~cm}\) has 100 turns of wire and carries a current, \(i=100 . \mathrm{mA} .\) It is free to rotate in a region with a constant horizontal magnetic field given by \(\vec{B}=(0.0100 \mathrm{~T}) \hat{x}\). If the unit normal vector to the plane of the coil makes an angle of \(30.0^{\circ}\) with the horizontal, what is the magnitude of the net magnetic torque acting on the coil? 27.61 At \(t=0\) an electron crosses the positive \(y\) -axis (so \(x=0\) ) at \(60.0 \mathrm{~cm}\) from the origin with velocity \(2.00 \cdot 10^{5} \mathrm{~m} / \mathrm{s}\) in the positive \(x\) -direction. It is in a uniform magnetic field. a) Find the magnitude and the direction of the magnetic field that will cause the electron to cross the \(x\) -axis at \(x=60.0 \mathrm{~cm}\). b) What work is done on the electron during this motion? c) How long will the trip take from \(y\) -axis to \(x\) -axis?

A straight wire of length \(2.00 \mathrm{~m}\) carries a current of \(24.0 \mathrm{~A} .\) It is placed on a horizontal tabletop in a uniform horizontal magnetic field. The wire makes an angle of \(30.0^{\circ}\) with the magnetic field lines. If the magnitude of the force on the wire is \(0.500 \mathrm{~N}\), what is the magnitude of the magnetic field?

A charged particle is moving in a constant magnetic field. State whether each of the following statements concerning the magnetic force exerted on the particle is true or false? (Assume that the magnetic field is not parallel or antiparallel to the velocity.) a) It does no work on the particle. b) It may increase the speed of the particle. c) It may change the velocity of the particle. d) It can act only on the particle while the particle is in motion. e) It does not change the kinetic energy of the particle.

A proton moving at speed \(v=1.00 \cdot 10^{6} \mathrm{~m} / \mathrm{s}\) enters a region in space where a magnetic field given by \(\vec{B}=\) \((-0.500 \mathrm{~T}) \hat{z}\) exists. The velocity vector of the proton is at an angle \(\theta=60.0^{\circ}\) with respect to the positive \(z\) -axis. a) Analyze the motion of the proton and describe its trajectory (in qualitative terms only). b) Calculate the radius, \(r\), of the trajectory projected onto a plane perpendicular to the magnetic field (in the \(x y\) -plane). c) Calculate the period, \(T,\) and frequency, \(f\), of the motion in that plane. d) Calculate the pitch of the motion (the distance traveled by the proton in the direction of the magnetic field in 1 period).

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