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| Velocities
of the same body in two frames of reference (see text). |
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As
the speed of one inertial frame of reference relative to another
is increased, its rods appear increasingly foreshortened and its
clocks more and more slowed down. As this relative speed approaches
c, both of these effects increase indefinitely. The relative
speed of the two frames cannot exceed c if light and other
electromagnetic phenomena are to travel at the speed c in
all directions when viewed from either frame of reference. Hence
the special theory of relativity forecloses relative speeds of frames
of reference greater than c. As an inertial frame of reference
can be associated with any material object in uniform nonrotational
motion, it follows that no material object can travel at a rate
of speed exceeding c.
This
conclusion is self-consistent only because under the Lorentz transformations
the velocity of a body with respect to one inertial frame of reference
is related to its velocity with respect to another frame not by
the Newtonian rule that the difference in velocities equals the
relative velocity between the two frames but by a more involved
formula, which takes into account the changes in scale length, in
clock time, and in simultaneity. If all velocities involved have
the same direction, then the velocity in one frame, u, is
related to the velocity in the other frame, u', by the expression
stating that u' equals the sum of u and v divided
by 1 plus the product of u and v divided by the square
of c:
As
long as neither u nor v exceeds the speed of light,
c, u' also will be less than c.
Variable
mass
The
mass of a material body is a measure of its resistance to a change
in its state of motion caused by a given force. The larger the mass,
the smaller the acceleration. If a material body is already moving
at a speed approaching the speed of light, it must offer increasing
resistance to any further acceleration so as not to cross the threshold
of c. Hence the special theory of relativity leads to the
conclusion that the mass of a moving body m is related to
the mass that it would have if at rest, m0, by
a formula in which m equals m0 divided
by the square root of one minus the fraction v2/c2:
This
changing value of the mass of the moving body, m, is called
the relativistic mass. As v approaches c, the figure
within the parentheses approaches zero and the mass m becomes
infinitely large.
The
relativistic mass formula may be interpreted as indicating that
the relativistic mass of a body exceeds its rest mass m0
by an amount that equals its kinetic energy E, divided by
c2: m - m0 = E/c2.
Hence the hypothesis that generally the energy is c2
times the mass, or E = mc2, and that energy
and mass are, in fact, equivalent physical concepts, differing only
by the choice of their units. This hypothesis has been verified
experimentally, in that all massive particles have been converted
into forms of energy (for instance, gamma radiation) and conversely
have been created out of pure energy. It was in part the recognition
of this relationship that led to research out of which grew the
technology of nuclear fission and fusion.
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Contents:
Introduction
The
special theory of relativity
Historical
background
Relativity
of space and time
Consequences
The
limiting character of the speed of light
Variable
mass
Invariant
intervals
The
"twin paradox"
Four-dimensional
space-time
The
general theory of relativity
Physical
origins
The
principle of equivalence
Curved
space-time
The
principles
The
mathematical expression
Confirmation
of the theory
Advance
of Mercury's perihelion
Gravitational
redshift
Optical
effects of gravitation
Gravitational
waves
Future
astrophysical tests
Conceptual
implications of general relativity
Schwarzschild's
solution of the field equations
Applications
of relativistic principles
Particle
accelerators
Relativistic
particle physics
Relativistic
cosmology
Modifications
of general relativity
Bibliography
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