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An important applications of binary systems is that under favorable
circumstances they provide one of the only ways to determine reliable masses for
stars.
Kepler's Laws and MassesThe determination of masses in binary systems
generally uses Kepler's 3rd Law,
( m1 +
m2 ) P2 = ( d1 + d2 ) 3 =
R3 where P is the orbital period, m1 and
m2 are the respective masses, and R = r1 + r2,
and the "seesaw equation" for the center of mass:
where R is the total separation between the centers of the two objects.
From the first of these equations, if the period P and the average separation
R are known, we can solve for the total mass M = m1 +
m2 of the binary system. Then, if we know enough about the orbits to
determine the distances d1 and d2 separately, the second
equation can be used to determine the individual masses m1 and
m2. (The above equations assume that the orbits are circular. If they
are more elliptical, the analysis is similar but becomes more complicated.)
Binary Masses with Limited InformationIn practical applications of mass
determination we are often faced with insufficient information to apply the
preceding method. This is typically because of some combination of two problems:
- We may not be able to map the orbits exactly (obviously true if the binary
is astrometric and we see only one star).
- Even if the orbits can be mapped, they correspond to the 2-dimensional
projections on the celestial sphere of the true 3-dimensional orbit and
further information is required to construct the true orbit.
In these
instances, we often can only determine only the sum of the masses rather than
the individual masses, or we may only be able to place limits on the
masses rather than actually determine them.
In the case of astrometric binaries, we can often find families of solutions
for masses or limits on the masses if certain assumptions are made about the
system such as the mass of the primary (which can often be estimated indirectly
from systematics of its luminosity and spectral type). |