Kepler's First Law of Planetary Motion:
The orbits of the planets are elliptical in shape with the sun at one focus.
Start by assuming a system of two bodies, the larger of which has mass M,
and the small of which has mass m, which are separated by a distance r.
Next assume an attractive force between the two bodies, F(r) which
depends solely on the distance separating the bodies.
The Principle of Least Action states that
must be an extrema.
From the conservation of energy,
which can be
re-written to show
A
look at a diagram of the situation
gives
To find where
this is an extrema, plug this into the Euler-Lagrange Equation, yielding
which means
where l
is a constant and turns out to be the total angular momentum of the system.
This can be re-written as
Squaring both
sides gives
Solving for q
’ yields
At this point
it is necessary to determine the form of U. Since the force governing the actions of the system is
gravity, the force is of the form
where k
is a constant. From the relation between force and
potential energy,
Plugging this
into the equation for q ’ gives This
differential equation can be solved
to give the result which is of the
form
It is easy to recognize that C
is just a rotation angle of the function, which means the shape of the orbit is
the same regardless of it’s value; it only affects to orientation of the
curve. For simplicity, choose C=0,
which gives
This expression for r is the generic form of a conic section with
one focus at the origin in polar coordinates.
The exact shape of the curve depends on the
eccentricity, e
,
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Background image courtesy of NASA's Planetary Photojournal.