Physics Help
Gravitational Force
Gravity
Gravitation is the
force of
attraction that exists between all particles with
mass
in the
universe. It is the force of gravity which is responsible for holding
objects onto the surface of
planets and, with
Newton's law of inertia is responsible for keeping objects in
orbit around one another.
"Gravity is the force that pulls you down." --
Merlin in
Disney's
The Sword in the Stone
Merlin was right, of course, but gravity does much more than
just hold you in your chair. It was the genius of
Isaac Newton to recognize that. Newton recalled in a late memoir that while
he was trying to figure out what kept the Moon in the sky, he saw an apple fall
to the ground in his orchard, and he realized that the
Moon
was not suspended in the sky, but continuously falling, like a cannon ball that
was shot so fast that it continuously misses the ground as it falls away due to
the curvature of the
Earth.
If one wishes to be precise, one should distinguish between
gravitation, the universal force of attraction, and gravity,
which is the
resultant, on the Earth's surface, of the attraction by the earth's masses,
and the centrifugal pseudo-force caused by the Earth's rotation. In casual
discussion, gravity and gravitation are often used
interchangeably.
By Newton's third law, any two objects exert equal and
oppositely directed gravitational pull on each other.
Speed of gravity: Einstein's theory of relativity predicts that the
speed of gravity (defined as the speed at which changes in location of a mass
are propagated to other masses) should be consistent with the speed of light. In
2002, the Fomalont-Kopeikin experiment produced measurements of the speed of
gravity which matched this prediction. However, this experiment has not yet been
widely peer-reviewed, and is facing criticism from those who claim that
Fomalont-Kopeikin did nothing more than measure the speed of light in a
convoluted manner.
Newton explains, "Every object in the
Universe attracts every other object with a
force directed along the
line
of centers for the two objects that is
proportional to the product of their masses and inversely proportional to
the
square of the separation between the two objects."
Newton eventually published his still famous law of universal
gravitation in his
Principia Mathematica as follows:
-
where:
-
F = gravitational force between two objects
-
m1 = mass of first object
-
m2 = mass of second object
-
r = distance between the objects
-
G =
universal constant of gravitation
Strictly speaking, this law applies only to point-like
objects. If the objects have spatial extent, the true force has to be found by
integrating the forces between the various points.
The above form is a simplified version. It is more properly
expressed as
vector
equation. (All quantities in bold represent vector
quantities in what follows.) The form below is vectorially complete:
-
where:
For the force on mass two, simply multiply
by -1.
The primary difference between the two formulations is that
the second form uses the difference in position to construct a vector that
points from one mass to the other, and then divides that vector by its length to
prevent it from changing the magnitude of the force.
It's important to understand that while Newton was able to
formulate his law of gravity in his monumental work, he was not comfortable with
it because he never, in his words, "assigned the cause of this power." In all
other cases, he used the phenomenon of motion to explain the origin of various
forces acting on bodies, but in the case of gravity, he was unable to
experimentally identify the motion that produces the force of gravity. Moreover,
he refused to even offer a hypothesis as to the cause of this force on grounds
that to do so was contrary to sound science.
He lamented the fact that 'philosophers have hitherto
attempted the search of nature in vain' for the source of the gravitational
force, as he was convinced 'by many reasons' that there were 'causes hitherto
unknown' that were fundamental to all the 'phenomena of nature.' These
fundamental phenomena are still under investigation and, though hypotheses
abound, the definitive answer is yet to be found. While it is true that
Einstein's hypotheses (see below) are successful in explaining the effects of
gravitational forces more precisely than Newton's in certain cases, he too never
'assigned the cause of this power,' in his theories. It is said that in
Einstein's equations, 'matter tells space how to curve, and space tells matter
how to move,' but this new idea, completely foreign to the world of Newton, does
not enable Einstein to assign the 'cause of this power' to curve space anymore
than the Law of Universal Gravitation enabled Newton to assign its cause. In his
own words:
-
I wish we could derive the rest of the phenomena of
nature by the same kind of reasoning from mechanical principles; for I am
induced by many reasons to suspect that they may all depend upon certain
forces by which the particles of bodies, by some causes hitherto unknown, are
either mutually impelled towards each other, and cohere in regular figures, or
are repelled and recede from each other; which forces being unknown,
philosophers have hitherto attempted the search of nature in vain.
If science is eventually able to discover the cause of the
gravitational force, Newton's wish could eventually be fullfiled as well.
The gravitational attraction of
protons is approximately a factor 1036 weaker than the
electromagnetic repulsion. This factor is independent of distance, because
both forces are inversely proportional to the square of the distance. Therefore
on an atomic scale mutual gravity is negligible. However, the main force beween
common objects and the earth and between celestial bodies is gravity; this is
due to the fact that they (at least one of the two) are electrically neutral to
a high degree: even if in both bodies there were a surplus or deficit of only
one electron for every 1018 protons and
neutrons this would already be enough to cancel gravity (or in the case of a
surplus in one and a deficit in the other: double the attraction).
The relative weakness of gravity can be demonstrated with a
small
magnet picking up pieces of
iron.
The small magnet is able to overwhelm the gravitational force of the entire
earth.
Gravity is small unless at least one of the two bodies is
large, but the small gravitational force exerted by bodies of ordinary size can
fairly easily be detected through experiments such as the
Cavendish torsion bar experiment.
A self-gravitating system is a system of masses kept together
by mutual gravity. An example is a
star.
Nobody knows for sure if Newton's recollection about the
apple was accurate, but his insight is the same nevertheless.
Philosophers had thought since the Greeks that the "natural" movement of
stars,
planets, the
Sun
and the Moon was circular,
Kepler established that orbits are actually
elliptical, but still thought that the movements of the planets was dictated
by some "divine force" emanated from the sun, but Newton realized that the same
force that causes a thrown rock to fall back to the Earth keeps the planets in
orbit of the Sun, and the Moon in orbit of the Earth.
Newton was not alone in making significant contributions to
the understanding of gravity. Before Newton,
Galileo Galilei corrected a common misconception, started by
Aristotle, that objects with different mass fall at different rates. To
Aristotle, it simply made sense that objects of different mass would fall at
different rates, and that was enough for him. Galileo, however, actually tried
dropping objects of different mass at the same time. Aside from differences due
to friction from the air, Galileo observed that all masses accelerate the same.
Using Newton's equation, F = ma, it is plain to us why:
-
The above equation says that mass m1 will
accelerate at
acceleration a1 under the force of gravity, but divide
both sides of the equation by m1 and:
-
Nowhere in the above equation does the mass of the falling
body appear. When dealing with objects near the surface of a planet, the change
in r divided by the initial r is so small that the
acceleration due to gravity appears to be perfectly constant. The acceleration
due to gravity on
Earth is usually called g, and its value is about 9.8 m/s2
(or 32 ft/s2). Galileo didn't have Newton's equations, though, so his
insight into gravity's proportionality to mass was invaluable, and possibly even
affected Newton's formulation on how gravity works.
However, across a large body, variations in r can
create a significant
tidal force.
Newton's formulation of gravity is quite accurate for most
practical purposes. It has a few problems with it though:
-
It assumes that changes in the gravitational force are
transmitted instantaneously when positions of gravitating bodies change.
However, this contradicts the fact that there exists a maximum velocity at
which signals can be transmitted (speed
of light in vacuum).
-
Assumption of absolute space and time contradicts
Einstein's theory of
Special relativity.
-
It predicts that light is deflected by gravity only half as
much as observed.
-
It does not explain
gravitational waves or
black holes.
-
Under newtonian gravity (with instantaneous transmission of
gravitational force), if the
Universe is
Euclidean, static, of uniform, average, positive density and infinite,
then the total gravitational force on a point is a divergent
series. In other words, newtonian gravity is inconsistent with a
Universe which is
Euclidean, static, of uniform, average, positive density and infinite.
For the first two of these reasons,
Einstein and
Hilbert developed a new theory of gravity called
General Relativity, published in
1915.
This theory predicts that the presence of matter "warps" the local space-time
environment, so that apparently "straight" lines through space and time have the
properties we think of "curved" lines as having.
Although General Relativity is, as a theory, more accurate
than Newton's law of gravity, it also requires a significantly more complicated
mathematical formalism. Instead of describing the effect of gravitation as a
"force", Einstein introduced the concept of curved
space-time in which bodies move along curved trajectories.
Today General Relativity is accepted as the standard
description of classical gravitational phenomena. (Alternative theories of
gravitation exist but are more complicated than General Relativity.) General
Relativity is consistent with all currently available measurements. For weak
gravitational fields and bodies moving at slow speeds at small distances,
Einstein's General Relativity gives almost exactly the same predictions as
Newton's law of gravitation. Crucial experiments that justified the adoption of
General Relativity over Newtonian gravity were the gravitational
redshift, the deflection of light rays by the Sun, and the
precession of the orbit of
Mercury.
More recent experimental confirmations of General Relativity
were gravitational waves from orbiting
binary stars, the existence of
neutron stars and black holes,
gravitational lensing, and the convergence of measurements in observational
cosmology to an approximately flat model of the observable
Universe, with a matter density parameter of approximately 30% of the
critical density and a
cosmological constant of approximately 70% of the critical density.
Gravity is the only one of the four
fundamental forces of nature that stubbornly refuses to be quantised (the
other three:
Electromagnetism, the
Strong Force, and the
Weak Force, can be quantised). Quantisation means that the force is measured
in discrete steps that cannot be reduced in size, no matter what; alternatively,
that gravitational interaction is trasmitted by particles called
gravitons. Scientists have theorized about the graviton for years, but have
been frustrated in their attempts to find a consistent
quantum theory for it. Many believe that
string theory holds a great deal of promise to unify general relativity and
quantum mechanics, but this promise has yet to be realized.
Home | Up | Gravitational Force | Electromagnetic Force | Weak Force | Strong Force
Physics Help, made by MultiMedia | Free content and software
This guide is licensed under the GNU
Free Documentation License. It uses material from the Wikipedia.
|