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In [[astronomy]], the '''binary mass function''' or simply '''mass function''' is a [[Function (mathematics)|function]] that constrains the [[mass]] of the unseen component (typically a [[star]] or [[exoplanet]]) in a single-lined spectroscopic [[binary star]] or in a [[planetary system]]. It can be calculated from [[Observation|observable]] quantities only, namely the [[orbital period]] of the binary system, and the peak [[radial velocity]] of the observed star. The velocity of one binary component and the orbital period provide (limited) information on the separation and gravitational
== Introduction ==
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The observed object of which the radial velocity can be measured is taken to be object 1 in this article, its unseen companion is object 2.
Let <math>M_{1}</math> and <math>M_{2}</math> be the stellar masses, with <math>M_{1} + M_{2} = M_\mathrm{tot}</math> the total mass of the binary system, <math>v_{1}</math> and <math>v_{2}</math> the orbital velocities, and <math>a_{1}</math> and <math>a_{2}</math> the distances of the objects to the center of mass
We start out with Kepler's third law, with <math>\omega_\mathrm{orb} = 2 \pi/P_\mathrm{orb}</math> the [[Angular frequency|orbital frequency]] and <math>G</math> the [[gravitational constant]],
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<math>GM_\mathrm{tot} = \omega_\mathrm{orb}^{2} a^{3}.</math>
Using the definition of the center of mass ___location, <math>M_{1} a_{1} = M_{2} a_{2}</math>,<ref name="karttunen" /> we can write
<math>a = a_{1} + a_{2} = a_{1} \left(1 + \frac{a_{2}}{a_{1}}\right) = a_{1} \left(1 + \frac{M_{1}}{M_{2}}\right) = \frac{a_{1}}{M_{2}} (M_{1} + M_{2}) = \frac{a_{1} M_\mathrm{tot}}{M_{2}}.</math>
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<math>f \approx M_{2}\ \mathrm{sin}^{3}i,</math>
and
In general, for any <math>i</math> or <math>M_{1}</math>,
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