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Fully stripped (all electrons removed) sulfur \(\left({ }^{32} \mathrm{~S}\right)\) ions are accelerated in an accelerator from rest using a total voltage of \(1.00 \cdot 10^{9} \mathrm{~V}\). \({ }^{32} \mathrm{~S}\) has 16 protons and 16 neutrons. The accelerator produces a beam consisting of \(6.61 \cdot 10^{12}\) ions per second. This beam of ions is completely stopped in a beam dump. What is the total power the beam dump has to absorb?

Short Answer

Expert verified
Answer: The total power the beam dump must absorb is approximately 1.69 x 10^4 W or 16.9 kW.

Step by step solution

01

Calculate the charge of the sulfur ion

Since sulfur has 16 protons and is fully stripped (meaning no electrons are present), the charge of one sulfur ion is the charge of 16 protons. The charge of one proton is \(1.60 \times 10^{-19} \mathrm{C}\). So the charge of the sulfur ion can be calculated as: \(q = 16 \times 1.60 \times 10^{-19} \mathrm{C} = 2.56 \times 10^{-18} \mathrm{C}\)
02

Calculate the kinetic energy of one ion

The potential energy gained by one ion from the given voltage is equal to the kinetic energy of the ion. We can determine the kinetic energy using the equation: \(KE = qV\), where \(q\) is the charge of the ion and \(V\) is the voltage. Therefore, \(KE = (2.56 \times 10^{-18} \mathrm{C})(1.00 \times 10^{9} \mathrm{V}) = 2.56 \times 10^{-9} \mathrm{J}\)
03

Calculate the kinetic energy of all ions per second

We know that the accelerator produces \(6.61 \times 10^{12}\) ions per second. So, the total kinetic energy of all ions per second will be: \(KE_{total} = (6.61 \times 10^{12} \text{ ions/s})(2.56 \times 10^{-9} \mathrm{J/ion}) = 1.69 \times 10^{4} \mathrm{J/s}\)
04

Find the total power that the beam dump has to absorb

Since power is defined as the amount of energy transferred per unit time, the total power that the beam dump has to absorb can be inferred from the total kinetic energy of all ions per second. In this case, the power is equal to: \(P = 1.69 \times 10^{4} \mathrm{J/s}\) So, the total power the beam dump must absorb is approximately \(1.69 \times 10^{4} \mathrm{W}\) or \(16.9 \mathrm{kW}\).

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Key Concepts

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

Ion Acceleration
In nuclear physics, ion acceleration is a crucial process where charged particles, or ions, are subjected to an electric field, rapidly increasing their velocity. Here, fully stripped sulfur ions with 16 protons are accelerated from rest across a voltage of 1 billion volts. This process involves transferring energy from the electric field to the ions, making them move faster.

Fully stripped ions mean they lack electrons, resulting in a positive charge equal to the sum of their protons' charges. These ions are directed through an accelerator which uses strong electric fields to push them to higher speeds. This acceleration is key in experiments and practical applications like cancer treatment with ion beams.

Ion accelerators are essential tools in modern science, allowing researchers to probe the structure of matter at a subatomic level and enabling the generation of high-energy beams.
Kinetic Energy Calculation
The concept of kinetic energy refers to the energy a particle possesses due to its motion. Ion acceleration involves converting electrical energy into kinetic energy, which can be calculated using the formula \( KE = qV \), where \( q \) is the charge of the ion and \( V \) is the accelerating voltage.

For a sulfur ion with a charge \( q = 2.56 \times 10^{-18} \mathrm{C} \) and a voltage of \( 1.00 \times 10^{9} \mathrm{V} \), the kinetic energy turns out to be \( 2.56 \times 10^{-9} \mathrm{J} \). This energy represents how much work was done on the ion to accelerate it.

Kinetic energy calculations are fundamental in understanding how ions move and interact, shaping fields such as particle physics and material science.
Beam Dump Power Absorption
When high-energy ions are stopped, as in a beam dump, they transfer their kinetic energy to the material of the beam dump, resulting in energy absorption. This absorbed energy is a form of power, measured in watts.

In this scenario, the accelerator produces \( 6.61 \times 10^{12} \) ions every second, each carrying \( 2.56 \times 10^{-9} \mathrm{J} \) of kinetic energy. Thus, the power absorbed by the beam dump is \( 1.69 \times 10^{4} \mathrm{J/s} \) or \( 16.9 \mathrm{kW} \).

The concept of power absorption is pivotal in ensuring that equipment doesn't overheat and functions safely. It also helps in designing effective thermal management systems to dissipate the absorbed energy.

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Most popular questions from this chapter

In which situation is the electric potential the highest? a) at a point \(1 \mathrm{~m}\) from a point charge of \(1 \mathrm{C}\) b) at a point \(1 \mathrm{~m}\) from the center of a uniformly charged spherical shell of radius \(0.5 \mathrm{~m}\) with a total charge of \(1 \mathrm{C}\) c) at a point \(1 \mathrm{~m}\) from the center of a uniformly charged rod of length \(1 \mathrm{~m}\) and with a total charge of \(1 \mathrm{C}\) d) at a point \(2 \mathrm{~m}\) from a point charge of \(2 \mathrm{C}\) e) at a point \(0.5 \mathrm{~m}\) from a point charge of \(0.5 \mathrm{C}\)

An electron moves away from a proton. Describe how the potential it encounters changes. Describe how its potential energy is changing.

A point charge \(Q\) is placed a distance \(R\) from the center of a conducting sphere of radius \(a,\) with \(R>a\) (the point charge is outside the sphere). The sphere is grounded, that is, connected to a distant, unlimited source and/or sink of charge at zero potential. (Neither the distant ground nor the connection directly affects the electric field in the vicinity of the charge and sphere.) As a result, the sphere acquires a charge opposite in sign to \(Q\), and the point charge experiences an attractive force toward the sphere. a) Remarkably, the electric field outside the sphere is the same as would be produced by the point charge \(Q\) plus an imaginary mirror-image point charge \(q\), with magnitude and location that make the set of points corresponding to the surface of the sphere an equipotential of potential zero. That is, the imaginary point charge produces the same field contribution outside the sphere as the actual surface charge on the sphere. Calculate the value and location of \(q\). (Hint: By symmetry, \(q\) must lie somewhere on the axis that passes through the center of the sphere and the location of \(Q .)\) b) Calculate the force exerted on point charge \(Q\) and directed toward the sphere, in terms of the original quantities \(Q, R,\) and \(a\) c) Determine the actual nonuniform surface charge distribution on the conducting sphere.

Derive an expression for electric potential along the axis (the \(x\) -axis) of a disk with a hole in the center, as shown in the figure, where \(R_{1}\) and \(R_{2}\) are the inner and outer radii of the disk. What would the potential be if \(R_{1}=0 ?\)

A deuterium ion and a tritium ion each have charge \(+e .\) What work is necessary to be done on the deuterium ion in order to bring it within \(10^{-14} \mathrm{~m}\) of the tritium ion? This is the distance within which the two ions can fuse, as a result of strong nuclear interactions that overcome electrostatic repulsion, to produce a helium-5 nucleus. Express the work in electron-volts.

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