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if possible could you tag some good video lectures may be feymann or any other good source..thanks...!!

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- Thread starter shivaniits
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Prove? This is like asking someone to prove Quantum Mechanics. Mathematically, there are a ridiculous number of consistent theories, so all we can do is fail to disprove it.

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mathman

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http://en.wikipedia.org/wiki/Special_relativity

http://en.wikipedia.org/wiki/Mass–energy_equivalence

Try either of the above.

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are there any good feymann lectures on special theory of relativity or quantum mechanics...???

thanks!!

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@mathman thanks i will try them!!

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In special relativity, time is just another dimension, just like spatial distance. The numerical value of the speed of light is a proportionality factor between time and length units. This identification causes a series of other identifications.

Speed becomes an angle between the time directions between two moving reference frames. This also nicely explains Lorentz transformations and relativistic speed composition.

Mass, momentum and energy are also identified. The proportionality factors between the standard units of these parameters are: momentum is mass times c and energy is mass times c squared. That's all.

Electric and magnetic potentials also undergo an unification into electromagnetic potential.

This is the basic idea of the special relativity. We live in a 4D space. Our common 3D physical properties turn out to be spatial or time-like components of 4-dimensional properties. Time and space are the same, but our standard unit system (say SI system) has different units for them. When we want to convert from time to space, we need to multiply the numerical value of the property by some proportionality factor, which is always some power of c, depending on the dimesionality of our property.

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Speed becomes an angle between the time directions between two moving reference frames. This also nicely explains Lorentz transformations and relativistic speed composition.

Mass, momentum and energy are also identified. The proportionality factors between the standard units of these parameters are: momentum is mass times c and energy is mass times c squared. That's all.

Electric and magnetic potentials also undergo an unification into electromagnetic potential.

This is the basic idea of the special relativity. We live in a 4D space. Our common 3D physical properties turn out to be spatial or time-like components of 4-dimensional properties. Time and space are the same, but our standard unit system (say SI system) has different units for them. When we want to convert from time to space, we need to multiply the numerical value of the property by some proportionality factor, which is always some power of c, depending on the dimesionality of our property.

because it what we perceive from different reference frames due to account of special relativity

and we can't say that

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mathman

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so can we say this conversion of E=mc^2 doesn't happen at all

because it what we perceive from different reference frames due to account of special relativity

and we can't say that

actually a some lump let say of m mass is vanishing(or more precisely should i say converting to energy)... doesn't really happen whatever we measure is due to special relativity effect!!

Utter nonsense! Pair production converts photons to electron-positron pairs. Nuclear fission or nuclear fusion convert mass to energy.

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The OP is asking whether we can prove it from more fundamental principles that have been established experimentally. The answer is yes, and that's exactly what Einstein did in his 1905 paper "Does the inertia of a body depend upon its energy content?," http://www.fourmilab.ch/etexts/einstein/E_mc2/www/

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You speak about convertingPair production converts photons to electron-positron pairs. Nuclear fission or nuclear fusion convert mass to energy.

OP was refering to

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OP was refering tototal massandtotal energyas I understand. These quantities never change for an isolated system and are always proportional to each other with a factor c^2.

The OP just asked about [itex]E=mc^2[/itex] in general. If the two sides of the equation were always simply defined as synonyms, then the equation would be vacuous. That's not what the equation expresses.

It's also not true that total mass is separately conserved. Mass isn't even additive. E.g., in Einstein's 1905 paper, the body that emitted the two light rays in opposite direction lost an amount of mass L/c

What's conserved isn't mass or energy separately but mass-energy.

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It is, in all known theories. In QM for example, it comes from Noether theorem and the trivial fact that Hamiltonian commutes with itself.It's also not true that total mass is separately conserved.

It is.Mass isn't even additive.

No, they don't. They have zeroE.g., in Einstein's 1905 paper, the body that emitted the two light rays in opposite direction lost an amount of mass L/c^{2}. Each light ray has zero mass.

You don't need a box for the inertia to be the same. The inertia (total mass) of the system will be equal to the sum of the total masses of each particle.The sum of the masses has been reduced by L/c^{2}. However, if you put the whole system, in its final state, inside a box, its inertia is the same as that of the original system, and unequal to the sum of the three masses.

What's conserved isn't mass or energy separately but mass-energy.

There are different physical quantities calles "mass" and "energy" and they are not the same despite they have similar names.

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DrGreg

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Utter nonsense! Pair production converts photons to electron-positron pairs. Nuclear fission or nuclear fusion convert mass to energy.

No, nuclear fission does not convert mass into energy.

It releases binding energy of a nucleus.

To me so far, E=mc

Conversion of Kg into Joules.

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I am aware, and that is why I always give the proper adjective here (rest, kinetic, potential, total).c^{2}).

This jargon is very misleading, by the way. Many non-specialists in the world have hard time understanding what all this actually means.

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It's also not true that total mass is separately conserved. Mass isn't even additive.

Classical inertial mass as defined by p=m·a is additive, the rest mass is not and both are conserved in isolated systems. Conversion of mass into energy or vice versa would violate this conservation as well as the conservation of energy.

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Classical inertial mass as defined by p=m·a is additive, the rest mass is not and both are conserved in isolated systems. Conversion of mass into energy or vice versa would violate this conservation as well as the conservation of energy.

However, the

Also, the real measurement of inertia is

I am amazed how poorly this topic is understood.

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Rest mass is not conserved. Consider an electron and a position annihilating into two photons. Before the annihilation, the rest mass is two times rest mass of an electron. After the annihilation, the rest mass of the system is zero.

The rest mass of the system is not zero. It is unchanged during the annihilation.

However, thetotal massof the system is conserved and is the same before and after the annihilation.

What is your definition for the "total mass"?

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Roughly speaking: rest mass, plus kinetic mass, plus potential mass. Equivalent definition: rest energy, plus kinetic energy, plus potential energy, divided by c^2.What is your definition for the "total mass"?

A free particle is characterized by 4 independent quantities: its total mass, and momentum. To convert from momentum to mass units, you have to divide it by c. These 4 numbers form a Lorentz vector called 4-momentum. Length of the 4-momentum is the rest mass, a Lorentz scalar.

The rest mass (scalar) is the same in any inertial reference frame. The total mass (and momentum) can change with reference frames. In a rest frame momentum of a particle is zero and the total mass equals the rest mass. In a moving frame momentum is nonzero and total mass increases by a factor "1 / √(1 - v^2/c^2)". This also has a beautiful geometrical explanation, as these are 4-momentum space and time coordinates in the new frame, respectively.

When you not care about Lorentz covariance, you can subtract total mass and rest mass and the result will be kinetic mass. When you multiply it by c^2, you get kinetic energy. In a small speed limit, it reduces to "m v^2 / 2". This is another way of looking at 4-momentum. It is not Lorentz-covariant, but it is preferred by some, possibly because of similarity to normal Newtonian physics.

To sum things up.

4D view:

- 4-momentum, a Lorentz vector.

- Rest mass, the length of the 4-momentum, a Lorentz scalar.

3D view:

- Momentum, space-like part of 4-momentum. It is a spatial vector.

- Total mass, time-like part of 4-momentum. It varies with speed.

- Rest mass, the same as in 4D view.

- Kinetic mass. It varies with speed. It is proportional to kinetic energy. When added to the rest mass, it gives the total mass.

Now, what it means to be conserved? Imagine a 4D spacetime with some process happening in it. Suppose we have an inertial frame. Take one moment (a space-like surface). Compute some quantity. Take some other moment. Is the quantity the same?

With this definition, 4-momentum is conserved. Total mass and momentum are also conserved, as they are components of the 4-momentu. No other quantity defined above is conserved.

Note that conservation is a different thing from Lorentz covariance. If we take some different inertial frame, momentum and total mass will be different. But they will still be conserved, that means they sum on each moment of the same reference frame will be the same.

Conservation of a quantity is its immunity to time

This is extremely important to understand, as a common mistake is comparing total mass values from different inertial frames on different moments and "proving" its non-conservation. Namely, the rest mass is equal to the total mass in some reference frame. Some people first consider the time evolution (with some reference frame defining the time direction), then unconsiously move to the rest frame of the particle. This is not right.

To sum things up, once again:

- 4-momentum is a Lorentz 4-vector. It changes covariantly with boosts and rotations.

- Rest mass is a Lorentz scalar. It does not change with boosts and rotations. This is pure mathematics.

- Total mass is a time component of the 4-momentum.

- 4-momentum is conserved, that means for any closed system it does not change with time translations (and space-like translations too, for that matter).

- Rest mass is

- Total mass is conserved, since it is a time component of the 4-momentum.

I wanted to write about potential energy too, but this is too much for today. I hope I was clear enough.

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Roughly speaking: rest mass, plus kinetic mass, plus potential mass. Equivalent definition: rest energy, plus kinetic energy, plus potential energy, divided by c^2.

That sounds like the classical inertial mass (also known as relativistic mass) but the potential energy is a problem because the potential energy between parts of the system is already part of its rest energy and the potential energy between the system and external systems is not part of the system only.

Now, what it means to be conserved? Imagine a 4D spacetime with some process happening in it. Suppose we have an inertial frame. Take one moment (a space-like surface). Compute some quantity. Take some other moment. Is the quantity the same?

This is given for rest mass as well as for the relativistic mass.

- #22

DrGreg

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Rest massis not conserved.

Actually the real problem here is that there's no universally agreed language for explaining this. "Conservation of (rest) mass" could be interpreted in one of two ways:I am amazed how poorly this topic is understood.

- Conservation of the sum of the rest masses of the particles of a system. This is not true.
- Conservation of the "invariant mass", or "system mass", or "rest mass", of the whole system. Invariant mass means
*E*/*c*^{2}where*E*is the total energy of the system relative to the frame in which the total momentum is zero, or equivalently [tex]\frac{\sqrt{\left( \Sigma E \right)^2 - \left| \Sigma \textbf{p} \right|^2 c^2}}{c^2}[/tex] in any frame. This type of conservation is true.

Much of the recent disagreement in this thread has been due to different contributors interpreting the language differently. I don't think they are disagreeing over the actual physics, just the terminology.

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Actually the real problem here is that there's no universally agreed language for explaining this. "Conservation of (rest) mass" could be interpreted in one of two ways:

- Conservation of the sum of the rest masses of the particles of a system. This is not true.

[...]

This makes no sense because rest mass is not additive. The sum of the rest masses of the particles of a system is not the rest mass of the system. The rest mass of the system is the mass of the system at rest.

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This is an Youtube video made by a physicist. It is made with simple drawing and it is easily understandable.

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This is an Youtube video made by a physicist. It is made with simple drawing and it is easily understandable.

Here is a dumb thought.

Say, I have a ball in my hand of mass 1 Kg.

I throw it with speed 20m/sec.

Its kinetic energy is 200J. Mass equivalent of this energy is

2.22x10

Can we say mass of the ball is increased by 2.22x10

In another words, mass of the moving ball is 1+2.22x10

Is this the mass increase we see in special relativity caused by speed?

In such case, it is not a physical increase of mass at all.

Also, then measurements of masses of planets etc are not rest masses.

There must be a big hole in my thinking.

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