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Relativistic Mass, Momentum, and Energy

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Relativistic Mass, Momentum, and Energy
Special relativity forces one to reconsider the concepts of mass, momentum, and energy, all of which are important constructs in Newtonian mechanics. Special relativity shows, in fact, that these concepts are all different aspects of the same physical quantity in much the same way that it shows space and time to be interrelated.
Given an object of invariant mass m0 traveling at velocity v the energy and momentum are given by
Relativistic energy
Relativistic energy

Relativistic momentum
Relativistic momentum

E – Energy
p – Momentum
m0 – initial mass
c – Speed of light


The speed of light in a vacuum is exactly 299,792,458 meters per second (or 1,079,252,848.8 km•h-1, which is approximately 186,282.397 miles per second, or 670,616,629.4 miles per hour; sometimes roughly 300,000 km per second)

where γ (the Lorentz factor) is given by
Lorentz factor
Lorentz factor


For velocities much smaller than those of light, γ can be approximated using a Taylor series expansion and one finds that
using a Taylor series expansion relativistic energy
using a Taylor series expansion relativistic momentum

Looking at the above formulas for energy, one sees that when an object is at rest (v = 0 and γ = 1) there is a non-zero energy remaining:

Einstein relationship for energy
Einstein's relativistic mass-energy relation
Einstein relativistic mass-energy relation
Einstein's relativistic mass-energy relation


Relativistic mass
On special relativity sometimes define a relativistic mass which increases as the velocity of a body increases.
Using the relativistic mass definition, the mass of an object may vary depending on the observer's inertial frame in the same way that other properties such as its length may do so.

For example, consider a body with an invariant mass m0 moving at some velocity relative to an observer's reference system. That observer defines the relativistic mass of that body as:
Relativistic mass
Relativistic mass