Understanding the Relationship Between Energy, Mass, and Momentum in Relativity

  • Thread starter Thread starter mysearch
  • Start date Start date
  • Tags Tags
    Energy-momentum
mysearch
Gold Member
Messages
523
Reaction score
0
Hi, I am trying to quickly resolve a fairly basic question that cropped when considering relativity. Classically, the total energy of a system is often described in term of 3 components:

Total Energy = Rest Mass + Kinetic + Potential

If I ignore potential energy, i.e. a particle moving in space far from any gravitational mass, then I assume the general form above can be reduced to:

[1] E_T = m_o c^2 + 1/2mv^2

Now m_o is the rest mass, while I assume [m] has to be described as the relative mass as a function of its velocity [v], i.e.

[2] m = \frac {m_o}{\sqrt{(1-v^2/c^2)}}

However, relativity also introduces the idea of relativistic momentum:

[4] p = mv = \frac {m_o v}{\sqrt{(1-v^2/c^2)}}

However, the following link show the definition of `Relativistic Energy in Terms of Momentum’: http://hyperphysics.phy-astr.gsu.edu/hbase/relativ/relmom.html#c4 which I have expanded to the following form:

[5] E_X^2 = m_o^2 c^4 + p^2c^2 = m_o^2 c^4 + m^2v^2c^2

Now my initial assumption was that [E_X \equiv E_T], but examination of equations [1] and [5] suggests that this cannot be the case. Could somebody explain my error or the difference in the implied energy of these 2 equations?

As a side issue, energy is a scalar quantity, while momentum is a vector quantity. I see how multiplying [p] by [c] gets us back to the units of energy, but was slightly unsure about the maths of mixing these quantities. Would appreciate any clarification of the issues raised. Thanks
 
Last edited by a moderator:
Physics news on Phys.org


Whilst you're initial assumption is correct, i.e. the total energy of a body is the sum of it's rest energy, kinetic energy and potential energy; your expression isn't. You're mixing classical and relativistic terms.

mysearch said:
E_T = m_o c^2 + 1/2mv^2

Note that E_k = \frac{1}{2}mv^2 is a strictly classical definition of kinetic energy, you can't simply substitute the relativistic mass for m. Instead, the relativistic kinetic energy is defined as E_k = \gamma m_0 c^2 - m_0 c^2 and is derivable from the expression for momentum.

mysearch said:
As a side issue, energy is a scalar quantity, while momentum is a vector quantity. I see how multiplying [p] by [c] gets us back to the units of energy, but was slightly unsure about the maths of mixing these quantities.

It is perfectly acceptable to multiply a vector by a scalar, in fact scalar multiplication is one of the operations which defines a vector space. Simply put, to multiply a vector by a scalar you simply multiply each of the components of the vector by the scalar quantity.

For example suppose we have a vector \bold{v} = \left(v_1, v_2, v_3\right) and a scalar a. Then:

a\cdot\bold{v} = a\cdot\left(v_1, v_2, v_3\right) = \left(a\cdot v_1, a\cdot v_2, a\cdot v_3\right)
 
[1] is wrong. You can't use the non-relativistic formula for kinetic energy. The kinetic energy is mc^2-m_0c^2.

Edit: D'oh, I was too slow again.

Mysearch, if you want to see a derivation, check out #15 in this thread. Read the stuff at the end first to see the difference between your notation and mine.
 
Last edited:


Hootenanny said:
Note that E_k = \frac{1}{2}mv^2 is a strictly classical definition of kinetic energy, you can't simply substitute the relativistic mass for m. Instead, the relativistic kinetic energy is defined as E_k = \gamma m_0 c^2 - m_0 c^2 and is derivable from the expression for momentum.
You can also take this expression for kinetic energy and do a Taylor series expansion about v = 0. When you do that you recover the classical definition of kinetic energy as the first term.
 
Many thanks for both quick responses.
I will follow up on the clarifications and link provided.
I have another issue, related to the conservation of energy,
but will raise it in a separate thread.
Thanks again.
 
Just wanted to say thanks again for the response in #2, #3 & #4. You were all right to point to equation [1], as [1/2mv^2] is only a low speed approximation.

Thanks for the clarification in #2 about scalars and vectors, I was aware that you could multiply a vector by a scalar, which gives you a vector, but as I was looking for an issue that would explain the 'apparent' discrepancy. The issue that I was worrying about was linked to the equation E^2 = m_o^2 c^4 + p^2c^2 and the concern (mistakenly) that a momentum vector was being added to scalar energy. Anyway, really appreciated the help.
 
OK, so this has bugged me for a while about the equivalence principle and the black hole information paradox. If black holes "evaporate" via Hawking radiation, then they cannot exist forever. So, from my external perspective, watching the person fall in, they slow down, freeze, and redshift to "nothing," but never cross the event horizon. Does the equivalence principle say my perspective is valid? If it does, is it possible that that person really never crossed the event horizon? The...
From $$0 = \delta(g^{\alpha\mu}g_{\mu\nu}) = g^{\alpha\mu} \delta g_{\mu\nu} + g_{\mu\nu} \delta g^{\alpha\mu}$$ we have $$g^{\alpha\mu} \delta g_{\mu\nu} = -g_{\mu\nu} \delta g^{\alpha\mu} \,\, . $$ Multiply both sides by ##g_{\alpha\beta}## to get $$\delta g_{\beta\nu} = -g_{\alpha\beta} g_{\mu\nu} \delta g^{\alpha\mu} \qquad(*)$$ (This is Dirac's eq. (26.9) in "GTR".) On the other hand, the variation ##\delta g^{\alpha\mu} = \bar{g}^{\alpha\mu} - g^{\alpha\mu}## should be a tensor...
ASSUMPTIONS 1. Two identical clocks A and B in the same inertial frame are stationary relative to each other a fixed distance L apart. Time passes at the same rate for both. 2. Both clocks are able to send/receive light signals and to write/read the send/receive times into signals. 3. The speed of light is anisotropic. METHOD 1. At time t[A1] and time t[B1], clock A sends a light signal to clock B. The clock B time is unknown to A. 2. Clock B receives the signal from A at time t[B2] and...
Back
Top