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(a) How much work must be done on a particle with mass \(m\) to accelerate it (a) from rest to a speed of \(0.090 c\) and (b) from a speed of \(0.900 c\) to a speed of \(0.990 c ?\) (Express the answers in terms of \(\left.m c^{2} .\right)\) (c) How do your answers in parts (a) and (b) compare?

Short Answer

Expert verified
The work done to accelerate the particle to \(v=0.090 c\) is simply \(KE_1\), and the work done to accelerate the particle from \(v = 0.900 c\) to \(v = 0.990 c\) is \(KE_2 - KE_1\), where \(KE_1\) and \(KE_2\) are the final kinetic energies in each case. The work needed to accelerate an already fast-moving particle is greater than the work needed to accelerate a particle from rest due to relativistic effects.

Step by step solution

01

Calculate the relativistic kinetic energy after the first acceleration

We are asked first for the kinetic energy of a particle with velocity \(v=0.090 c\). So, we'll substitute \(v=0.090 c\) into the relativistic KE formula: \(KE_1 = m c^2 (\frac{1}{\sqrt{1 - \left(\frac{0.090 c}{c}\right)^2}} - 1)\). Simplifying the velocity ratio leaves us with: \(KE_1 = m c^2 (\frac{1}{\sqrt{1 - 0.090^2 }} - 1)\).
02

Calculate the relativistic kinetic energy after the second acceleration

Similarly, the kinetic energy of the particle when it reaches \(v = 0.990 c\) is given by: \(KE_2 = m c^2 (\frac{1}{\sqrt{1 - \left(\frac{0.990 c}{c}\right)^2 }} - 1)\), which simplifies to: \(KE_2 = m c^2 (\frac{1}{\sqrt{1 - 0.990^2 }} - 1)\).
03

Subtract the initial kinetic energies from the final kinetic energies for both cases

When the particle is at rest, its initial kinetic energy is zero. So the work done on the particle to accelerate it to \(v=0.090 c\) is simply \(KE_1\). To find the work required to accelerate the particle from \(v = 0.900 c\) to \(v = 0.990 c\), subtract the initial kinetic energy at \(v = 0.900 c\) from the kinetic energy at \(v = 0.990 c\). This gives us the change in kinetic energy, which equals the work done.
04

Compare the work done in both cases

You will find if you solve for both cases that the work done to accelerate the particle when it's already travelling at a high velocity is more than the work done to accelerate the particle from rest to a lower velocity. This is a concept from relativity—more work is needed to accelerate a particle already moving at a high speed close to the speed of light \(c\) than is required to accelerate a particle from rest.

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Key Concepts

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

Work-Energy Principle
The work-energy principle is a fundamental concept in physics that relates the work done on an object to the change in its kinetic energy. It states that the work done by all forces acting on a particle equals the change in the particle's kinetic energy.
When dealing with relativistic speeds, this principle still applies, but with adjustments for relativistic effects. Conventional kinetic energy calculations assume that mass is constant. However, at speeds approaching the speed of light, an object's mass effectively increases (according to relativity), which affects how we calculate the kinetic energy.
  • At lower speeds, kinetic energy is calculated as \[ KE = \frac{1}{2}mv^2 \].
  • At relativistic speeds, it is calculated as \[ KE = mc^2 \left(\frac{1}{\sqrt{1 - \left(\frac{v}{c}\right)^2}} - 1\right) \].
In both scenarios, the work done on the particle is the change in kinetic energy. This means that if a particle accelerates, the work required depends not only on its change in speed but also on the relativistic changes in its properties.
Special Relativity
Special relativity, a theory introduced by Albert Einstein, revolutionized the way we understand time, space, and energy. It deals with objects moving at significant fractions of the speed of light and introduces the idea that the laws of physics are the same for all observers, regardless of their constant velocity.
One major revelation of special relativity is the concept of time dilation and length contraction. However, for kinetic energy and work done on particles, the more relevant outcome is the way mass and energy relate through the equation:
  • \( E = mc^2 \)
This equation implies that mass and energy are interchangeable. As objects speed up and approach the speed of light, an increase in their kinetic energy also effectively increases their relativistic mass.
This increase means that more energy is needed to keep accelerating the object as it moves faster, leading to the understanding that nothing can exceed the speed of light because it would require infinite energy.
Particle Acceleration
Particle acceleration involves increasing a particle's velocity using various methods. At high speeds, especially relativistic speeds, this becomes an intricate task due to energy requirements imposed by relativistic physics.
When accelerating particles such as electrons or protons, devices like particle accelerators are used. These devices employ electric fields to propel charged particles to high speeds, often close to the speed of light.
At low velocities, increasing a particle's speed primarily requires overcoming inertia. However, as speeds increase and approach the speed of light, additional forces are required to continue accelerating the particle due to their increasing kinetic energy and relativistic mass.
Key points in particle acceleration:
  • Initial accelerations require less energy as they take particles from rest to moderate speeds.
  • As speeds increase, the energy needed for further acceleration surges significantly due to relativistic effects.
  • This principle is evident in systems like the Large Hadron Collider, where protons are pushed to near-light speeds.
Thus, particle acceleration is an exciting field that brings together electric and magnetic field technologies with profound implications of special relativity.

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Most popular questions from this chapter

The net force \(\vec{F}\) on a particle of mass \(m\) is directed at \(30.0^{\circ}\) counterclockwise from the \(+x\) -axis. At one instant of time, the particle is traveling in the \(+x\) -direction with a speed (measured relative to the earth) of \(0.700 c .\) At this instant, what is the direction of the particle's acceleration?

What is the speed of a particle whose kinetic energy is equal to (a) its rest energy and (b) five times its rest energy?

Spaceship \(A\) moves past the earth at \(0.80 c\) to the west. Spaceship \(B\) approaches \(A,\) moving to the east. Both spaceship crews measure their relative speed of approach to be \(0.98 c .\) What mass would the crews of both spaceships measure for the standard kilogram, kept at rest on the earth, (a) according to classical physics and (b) according to the special theory of relativity?

The positive muon \(\left(\mu^{+}\right),\) an unstable particle, lives on average \(2.20 \times 10^{-6} \mathrm{~s}\) (measured in its own frame of reference) before decaying. (a) If such a particle is moving, with respect to the laboratory, with a speed of \(0.900 c\), what average lifetime is measured in the laboratory? (b) What average distance, measured in the laboratory, does the particle move before decaying?

Quarks and gluons are fundamental particles that will be discussed in Chapter \(44 .\) A proton, which is a bound state of two up quarks and a down quark, has a rest mass of \(m_{\mathrm{p}}=1.67 \times 10^{-27} \mathrm{~kg}\). This is significantly greater than the sum of the rest mass of the up quarks, which is \(m_{\mathrm{u}}=4.12 \times 10^{-30} \mathrm{~kg}\) each, and the rest mass of the down quark, which is \(m_{\mathrm{d}}=8.59 \times 10^{-30} \mathrm{~kg} .\) Suppose we (incorrectly) model the rest energy of the proton \(m_{\mathrm{p}} c^{2}\) as derived from the kinetic energy of the three quarks, and we split that energy equally among them. (a) Estimate the Lorentz factor \(\gamma=\left(1-v^{2} / c^{2}\right)^{-1 / 2}\) for each of the up quarks using Eq. \((37.36) .\) (b) Similarly estimate the Lorentz factor \(\gamma\) for the down quark. (c) Are the corresponding speeds \(v_{\mathrm{u}}\) and \(v_{\mathrm{d}}\) greater than \(99 \%\) of the speed of light? (d) More realistically, the quarks are held together by massless gluons, which mediate the strong nuclear interaction. Suppose we model the proton as the three quarks, each with a speed of \(0.90 c,\) with the remainder of the proton rest energy supplied by gluons. In this case, estimate the percentage of the proton rest energy associated with gluons. (e) Model a quark as oscillating with an average speed of \(0.90 c\) across the diameter of a proton, \(1.7 \times 10^{-15} \mathrm{~m}\). Estimate the frequency of that motion.

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