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At what speed is a particle's total energy twice its rest energy?

Short Answer

Expert verified
The particle's speed needs to be \(\frac{\sqrt{3}}{2}\) the speed of light for its total energy to be twice its rest energy.

Step by step solution

01

Understand the equation

Remember that the total energy of a relativistic particle can be stated as \(E = \gamma m_0c^2\) where \(\gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}}\), \(m_0\) is the particle's rest mass, \(c\) is the speed of light, and \(v\) is the particle's velocity.
02

Establish the relation between total and rest energy

We are given that the total energy is twice the rest energy. This can be written in equation form as \(2m_0c^2 = \gamma m_0c^2\). Cancel out the common terms to get \(\gamma = 2\).
03

Solve for velocity

Substitute the value of \(\gamma\) into the equation \(\gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}}\). Solve this equation for \(v\), which gives \(v = \frac{\sqrt{3}}{2}c\).

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Key Concepts

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

Rest Energy
Rest energy is the energy that an object possesses due to its mass when it is at rest. This fundamental concept in physics is encapsulated by Einstein's famous equation, \(E_0 = m_0c^2\), where \(E_0\) symbolizes the rest energy, \(m_0\) is the rest mass of the object, and \(c\) represents the speed of light in a vacuum. Discovered as a part of his Theory of Relativity, Einstein showed that mass and energy are interchangeable, marking a new era in understanding the intricacies of mass-energy equivalence. For stationary particles, this rest energy is their total energy content, as they lack kinetic energy.

Understanding rest energy is pivotal in modern physics as it underscores the immense energy potential of even small amounts of mass. This principle is the basis for technologies like nuclear power, where splitting or combining atomic nuclei releases significant energy compared to the rest mass of the particles involved.
Total Energy of a Particle
When we speak of the total energy of a particle, we refer to the sum of its rest energy and the energy due to its motion, known as kinetic energy. This concept becomes especially interesting and complex when particles move at speeds close to the speed of light, necessitating a relativistic view. Here, the equation \(E = \gamma m_0c^2\) defines the total energy of a particle, where \(E\) is the total energy, \(\gamma\) is the Lorentz factor that accounts for relativistic effects, \(m_0\) is the rest mass, and \(c\) stands for the speed of light.

As particles accelerate, their kinetic energy increases, and so does their total energy. At speeds significant enough to invoke the Lorentz factor, which applies to relativistic velocities, the total energy grows more rapidly than it would under classic Newtonian physics. This leads to the fascinating result that as a particle's velocity approaches the speed of light, its total energy tends toward infinity, making it impossible to reach or exceed the speed of light with finite energy.
Speed of Light
The speed of light, denoted as \(c\), is a fundamental constant in physics, acting as the ultimate speed limit for energy, information, and matter in the universe. In the vacuum of space, light travels at approximately 299,792,458 meters per second. This constancy of \(c\) irrespective of the observer's frame of reference is a cornerstone of Einstein's Theory of Special Relativity.

In the realm of relativistic physics, the speed of light connects space and time, influencing the energy, momentum, and mass of moving objects. It also leads to intriguing phenomena such as time dilation and length contraction, which are experienced at relativistic speeds. Due to its pivotal role, the speed of light is utilized in the calculations of energy and momentum for both stationary and moving particles, tying together the very fabric of space-time.
Lorentz Factor
The Lorentz factor, often represented by the Greek letter \(\gamma\), is critical in adjusting physics equations for relativistic effects when dealing with high-velocity scenarios. It is defined by the equation \(\gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}})\), where \(v\) is the velocity of an object and \(c\) is the speed of light. As the velocity of an object increases and begins to approach the speed of light, the Lorentz factor increases significantly.

Importantly, the Lorentz factor shows up in numerous equations in relativity, including those for time dilation, length contraction, and the calculation of total energy, signifying how much an object's relative motion affects its properties as observed from different frames of reference. This factor is also crucial in our understanding of the massive energy demands required to accelerate an object as it moves faster and becomes subject to relativistic effects.

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Most popular questions from this chapter

A very fast pole vaulter lives in the country. One day, while practicing, he notices a 10.0 -m-long barn with the doors open at both ends. He decides to run through the barn at \(0.866 c\) while carrying his 16.0 -m-long pole. The farmer, who sees him coming, says. "Ahal!This guy's pole is length contracted to \(8.0 \mathrm{m}\) There will be a short interval of time when the pole is entirely inside the barn. If I'm quick, I can simultaneously close both barn doors while the pole vaulter and his pole are inside." The pole vaulter, who sees the farmer beside the barn, thinks to himself, "That farmer is crazy. The barn is length contracted and is only \(5.0 \mathrm{m}\) long. My 16.0 -m-long pole cannot fit into a \(5.0-\mathrm{m}-\) long barn. If the farmer closes the doors just as the tip of my pole reaches the back door, the front door will break off the last \(11.0 \mathrm{m}\) of my pole."

An astronaut travels to a star system 4.5 ly away at a speed of 0.9c. Assume that the time needed to accelerate and decelerate is negligible. a . How long does the journey take according to Mission Control on earth? b. How long does the journey take according to the astronaut? c. How much time elapses between the launch and the arrival of the first radio message from the astronaut saying that she has arrived?

A quarter-pound hamburger with all the fixings has a mass of \(200 \mathrm{g}\). The food energy of the hamburger (480 food calories) is \(2 \mathrm{MJ}.\) a. What is the energy equivalent of the mass of the hamburger? b. By what factor does the energy equivalent exceed the food energy?

An event has spacetime coordinates \((x, t)=(1200 \mathrm{m}, 2.0 \mu \mathrm{s})\) in reference frame S. What are the event's spacetime coordinates (a) in reference frame \(\mathbf{S}^{\prime}\) that moves in the positive \(x\) -direction at \(0.8 c\) and \((b)\) in reference frame \(S^{\prime \prime}\) that moves in the negative \(x\) -direction at \(0.8 c ?\)

The diameter of the solar system is 10 light hours. A spaceship crosses the solar system in 15 hours, as measured on earth. How long, in hours, does the passage take according to passengers on the spaceship? Hint: \(c=1\) light hour per hour.

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