Proving Relativistic Kinetic Energy: (1/2)*(gamma)mv^2

In summary, relativistic mass increases with velocity, but invariant mass remains the same regardless of speed. This discrepancy is resolved using the work-energy theorem.
  • #1
asdf1
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0
How do you prove that (1/2)*(gamma)mv^2 doen't equal the kinetic energy of a particle moving at relativistic speeds?
 
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  • #2
Simply because

[tex] E_{kin}=m_{0}c^{2}\left(\gamma-1\right) [/tex]

,which is different from your [itex] \frac{1}{2} \gamma m_{0}v^{2} [/itex]...?

Daniel.
 
  • #3
asdf1 said:
How do you prove that (1/2)*(gamma)mv^2 doen't equal the kinetic energy of a particle moving at relativistic speeds?
... yet another example why relativistic mass was a bad idea.

Mass doesn't change with speed.
[tex]E_{K} = (\gamma -1)mc^{2}[/tex]
 
  • #4
How so mass does not change with speed? I thought that as a particle approaches the speed of light then it must lose mass. What is it i got wrong here?
 
  • #5
There are two sorts of mass. One of them, called invariant mass, stays constant regardless of velocity and is a property of the particle itself (it doesn't depend on the particles state of motion).

This is preferred by many, probably even most, people, but there are a few vocal people who prefer the other sort of mass, relativistic mass.

Relativistic mass _increases_ with velocity according to the formula

[itex]m_r = \gamma m_0[/itex]

where [itex]m_r[/itex] is the relativistic mass, [itex]m_0[/itex] is the invariant mass, and [itex]\gamma = \frac{1}{\sqrt{1-(v/c)^2}}[/itex] depends on the velocity of the particle.

For some more information, see for instance the sci.physics.faq "Does mass change with velocity".

http://math.ucr.edu/home/baez/physics/Relativity/SR/mass.html
 
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  • #6
Trilairian said:
... yet another example why relativistic mass was a bad idea.

Mass doesn't change with speed.
[tex]E_{K} = (\gamma -1)mc^{2}[/tex]
This question has absolutely nothing to do with the great idea of relativistic mass.

asdf1 - Its a matter of calculation. Simply calculate the kinetic energy and you'll obtain

[tex]K = (\gamma - 1)m_0 c^2[/tex]

I worked out the calculation based on the work-energy theorem and placed them online at - http://www.geocities.com/physics_world/sr/work_energy.htm

Pete
 
  • #7
wow! thank you very much! :)
 

Related to Proving Relativistic Kinetic Energy: (1/2)*(gamma)mv^2

1. What is relativistic kinetic energy?

Relativistic kinetic energy is the energy possessed by an object due to its motion, taking into account the effects of special relativity. It is described by the equation (1/2)*(gamma)mv^2, where gamma is the Lorentz factor and v is the velocity of the object.

2. How is the equation for relativistic kinetic energy derived?

The equation (1/2)*(gamma)mv^2 can be derived from the relativistic energy equation, E = (gamma)mc^2, where m is the mass of the object and c is the speed of light. By solving for v and substituting it into the classical kinetic energy equation, (1/2)mv^2, we arrive at the equation for relativistic kinetic energy.

3. What is the difference between classical and relativistic kinetic energy?

Classical kinetic energy only takes into account the mass and velocity of an object, while relativistic kinetic energy also considers the effects of special relativity, such as time dilation and length contraction. At low speeds, the two equations are nearly identical, but at high speeds, the relativistic equation becomes more accurate.

4. How is relativistic kinetic energy relevant in modern science?

Relativistic kinetic energy plays a crucial role in many areas of modern science, including particle physics, nuclear energy, and astrophysics. It allows us to accurately calculate the energy and behavior of particles traveling at high speeds, which is essential in understanding the fundamental laws of the universe.

5. Can relativistic kinetic energy be observed or measured?

Yes, relativistic kinetic energy can be observed and measured in various experiments and real-world scenarios. For example, the Large Hadron Collider at CERN accelerates particles to nearly the speed of light, allowing scientists to study the effects of relativistic kinetic energy. Additionally, the energy released in nuclear reactions, such as in nuclear power plants, is a result of the conversion of mass to energy, including relativistic kinetic energy.

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