Close both component orbits around a common center
Both members of a binary respond to the same mutual gravitational force, but their accelerations differ inversely with mass. Neither body must remain fixed. In the center-of-mass frame their position vectors are opposite and obey M₁r₁=M₂r₂. The more massive component follows the smaller orbit, while both complete a cycle in the same period.
Learning outcome: Vary secondary mass fraction at fixed relative axis, then vary axis at fixed fraction. Close the radius sum, mass-weighted position and opposite momenta, and identify an observation that distinguishes barycenter from photocenter.
Starting recap
Retain relative versus barycentric geometry, time versus angle, fitted versus instantaneous velocity and complete energy/angular-momentum boundaries.
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At a=4 AU and secondary fraction 0.25, masses are 3 and 1 solar masses, radii 1 and 3 AU, and period 4 years. Speeds are π/2 and 3π/2 AU/year. Position balance is −3×1+1×3=0; opposite momentum magnitudes are each 3π/2.
Open the experimentPredict
Does the heavier star follow the larger or smaller path around the common center?
Experiment
Vary secondary mass fraction at fixed relative axis, then vary axis at fixed fraction. Close the radius sum, mass-weighted position and opposite momenta, and identify an observation that distinguishes barycenter from photocenter.
Close binary positions and momenta around the common center
Worked teaching model · synthetic values · Original circular binary total mass 4 solar masses, conventional P²=a³/M. Primary axis=a f, secondary axis=a(1−f); both have the same period. Displayed velocities are opposite tangential directions at the shown phase; no mass-luminosity assumption.
Reset keeps your prediction, captures and practice history.
The heavier component follows the smaller barycentric orbit while both share one period.
Their relative separation is the sum of the two barycentric radii. Opposite momenta cancel in the center-of-mass frame; equal gravitational force does not imply equal acceleration, speed or radius. Brightness is not used to assign mass.
| Quantity | Value | Unit |
|---|---|---|
| Primary mass | 3 | solar masses |
| Secondary mass | 1 | solar masses |
| Primary barycentric radius | 1 | AU |
| Secondary barycentric radius | 3 | AU |
| Common period | 4 | years |
| Primary tangential speed | 1.570796 | AU/year |
| Secondary tangential speed | 4.712389 | AU/year |
| Signed center-of-mass numerator | 0 | solar mass AU |
| Signed momentum sum | 0 | solar mass AU/year |
These original models are not measured orbit records or operational mission instructions. Retain the frame, assumptions and missing evidence before interpreting a real system.
The heavier component follows the smaller barycentric orbit while both share one period.
Their relative separation is the sum of the two barycentric radii. Opposite momenta cancel in the center-of-mass frame; equal gravitational force does not imply equal acceleration, speed or radius. Brightness is not used to assign mass.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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At relative a=2 AU and equal masses, find component radii, common period and speeds. Compare the relative orbital axis with either component radius.
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