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In a proton accelerator used in elementary particle physics experiments, the trajectories of protons are controlled by bending magnets that produce a magnetic field of 4.80 T. What is the magnetic-field energy in a 10.0 -cm' volume of space where \(B=4.80 \mathrm{T} ?\)

Short Answer

Expert verified
The magnetic-field energy is approximately 9.16 Joules.

Step by step solution

01

Understanding the Formula

The energy stored in a magnetic field within a given volume can be calculated using the formula \(U_B = \frac{1}{2\mu_0} B^2 V\) where \(U_B\) is the magnetic energy, \(B\) is the magnetic field strength, \(V\) is the volume, and \(\mu_0\) is the permeability of free space, approximately \(4\pi \times 10^{-7} \, \text{T} \cdot \text{m/A}\).
02

Converting Units

The volume provided is 10.0 cm³. First, convert this volume into cubic meters because the SI unit for volume in this context is meters. Therefore, \(10.0 \, \text{cm}^3 = 10.0 \times 10^{-6} \, \text{m}^3\).
03

Calculating Magnetic Energy

Using the formula \(U_B = \frac{1}{2\mu_0} B^2 V\), substitute the values \(B = 4.80 \, \text{T}\), \(\mu_0 = 4\pi \times 10^{-7} \, \text{T} \cdot \text{m/A} \), and \(V = 10.0 \times 10^{-6} \, \text{m}^3\). This gives: \(U_B = \frac{1}{2 \times 4\pi \times 10^{-7}} (4.80)^2 (10.0 \times 10^{-6})\).
04

Performing the Calculation

Calculate \(B^2 = (4.80)^2 = 23.04\). Then, \(\frac{1}{2 \times 4\pi \times 10^{-7}} = \frac{1}{8\pi \times 10^{-7}}\). This value is approximately \(3.9785 \times 10^{5}\). Finally, calculate \(U_B \approx 3.9785 \times 10^{5} \times 23.04 \times 10^{-6}\).
05

Conclusion

The magnetic field energy is calculated as approximately \(9.164 \, \text{Joule}\).

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Key Concepts

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

Proton Accelerator
A proton accelerator is a device that uses electromagnetic fields to propel charged particles, like protons, to high speeds. These machines are fundamentally important in the field of particle physics, as they allow scientists to examine the fundamental components of matter. Proton accelerators are used in a variety of applications, including research, medicine, and industry.
  • In research, particularly elementary particle physics, they help in probing the properties of atoms, nuclei, and the particles that constitute them, by smashing particles at nearly the speed of light.
  • In medicine, accelerators are used in cancer treatment through a method known as proton therapy, which targets tumors with high precision.
  • In industry, they can be used to produce materials with specific properties.

Protons are accelerated using magnetic and electric fields, with the focus on controlling their direction and speed. The intense energy levels achieved allow the particles to overcome barriers and make new reactions possible.
Bending Magnets
Bending magnets are a critical component in the function of a proton accelerator. These magnets generate magnetic fields that can alter the paths of moving charged particles, such as protons, within the accelerator.
  • Function: They are designed to change the trajectory of the particles without altering their speed. By adjusting the magnetic field, scientists can precisely control the pathways, making sure protons follow the intended route within the accelerator.
  • Design: Typically composed of magnetized materials wrapped around bends in the accelerator, guiding protons to their specific points of collision.
  • Role: Essential in ensuring that high-energy protons are directed accurately, thus maximizing efficiency and effectiveness in creating the desired experimental conditions.

By carefully controlling these magnets, accelerators can achieve consistent and repeatable results, allowing for high-purity scientific experiments.
Magnetic Field Strength
Magnetic field strength, denoted as \(B\), represents the intensity of a magnetic field in a given area. This measure is critical in proton accelerators as it influences how particles like protons are guided and controlled.
The unit of magnetic field strength is Tesla (T), which is a measure of the concentration of magnetic flux. In the context of the exercise, a field strength of 4.80 T is quite strong, indicating a powerful magnetic field capable of significantly altering the path of protons.
  • High magnetic field strengths are necessary in accelerators to create the force needed to bend the trajectory of fast-moving protons.
  • These forces help ensure that protons reach the necessary energy and precise location for intended collisions or interactions.
  • Magnetic field strength must be carefully monitored and adjusted to maintain performance and achieve experimental objectives.

Accurately understanding and controlling this parameter ensures that complex experiments can be conducted reliably.
Permeability of Free Space
The permeability of free space, represented by the symbol \(\mu_0\), is a fundamental constant that measures the ability of a vacuum to support a magnetic field. It is used in calculations involving magnetic forces and fields, such as those in proton accelerators.
  • The value of \(\mu_0\) is approximately \(4\pi \times 10^{-7} \, \text{T}\cdot\text{m/A}\).
  • This constant plays a vital role when determining the energy stored in a magnetic field, as shown in the solution formula \(U_B = \frac{1}{2\mu_0} B^2 V\).
  • It acts as a bridge between magnetic field strength, volume, and energy, allowing scientists to calculate how much energy is involved in a specific magnetic setup.

Understanding \(\mu_0\) is crucial for physicists when designing and operating magnetic systems in accelerators, ensuring the necessary conditions for experimental research are met efficiently and safely.

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Most popular questions from this chapter

A coil has 400 turns and self-inductance 4.80 \(\mathrm{mH}\) The current in the coil varies with time according to \(i=(680 \mathrm{mA}) \cos (\pi t / 0.0250 \mathrm{s})\) . (a) What is the maximum emf induced in the coil? (b) What is the maximum average flux through each turn of the coil? (c) At \(t=0.0180\) s, what is the magnitude of the induced emf?

A \(18.0-\mu \mathrm{F}\) capacitor is placed across a 22.5 \(\mathrm{V}\) batter for several seconds and is then connected across a \(12.0-\mathrm{mH}\) inductor that has no appreciable resistance. (a) After the capacitor and inductor are connected together, find the maximum current in the circuit. When the current is a maximum, what is the charge on the capacitor? (b) How long after the capacitor and inductor are connected together does it take for the capacitor to be completely discharged for the first time? For the second time? (c) Sketch graphs of the charge on the capacitor plates and the current through the inductor as functions of time.

One solenoid is centered inside another. The outer one has a length of 50.0 \(\mathrm{cm}\) and contains 6750 coils, while the coaxial inner solenoid is 3.0 \(\mathrm{cm}\) long and 0.120 \(\mathrm{cm}\) in diameter and contains 15 coils. The current in the outer solenoid is changing at 49.2 A/s. (a) What is the mutual inductance of these solenoids? (b) Find the emf induced in the innner solenoid.

An inductor is connected to the terminals of a battery that has an emf of 12.0 \(\mathrm{V}\) and negligible internal resistance. The current is 4.86 \(\mathrm{mA}\) at 0.940 \(\mathrm{ms}\) after the connection is completed. After a long time the current is 6.45 \(\mathrm{mA} .\) What are (a) the resistance \(R\) of the inductor and (b) the inductance \(L\) of the inductor?

A solenoidal coil with 25 turns of wire is wound tightly around another coil with 300 turns (see Example 30.1\() .\) The inner solenoid is 25.0 \(\mathrm{cm}\) long and has a diameter of 2.00 \(\mathrm{cm} .\) At a certain time, the current in the inner solenoid is 0.120 \(\mathrm{A}\) and is increasing at a rate of \(1.75 \times 10^{3} \mathrm{A} / \mathrm{s}\) . For this time, calculate: (a)the average magnetic flux through each turn of the inner solenoid; (b) the mutual inductance of the two solenoids; (c) the emf induced in the outer solenoid by the changing current in the inner solenoid.

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