\(\boldsymbol{a}\text{(}t\text{)}\) is the acceleration (\(\frac{\text{m}}{\text{s}^{2}}\))
Notes
The net force \(\boldsymbol{F}\) on a body is proportional to the acceleration \(\boldsymbol{a}\text{(}t\text{)}\) of the body, where \(m\) denotes the mass of the body as the constant of proportionality.
\({\boldsymbol{F}_{1}}\) is the force exerted by the first body (on another body) (\({\text{N}}\))
\({\boldsymbol{F}_{2}}\) is the force exerted by the second body (on another body) (\({\text{N}}\))
Notes
Every action has an equal and opposite reaction. In other words, the force \({\boldsymbol{F}_{1}}\) exerted on the second rigid body by the first is equal in magnitude and in the opposite direction to the force \({\boldsymbol{F}_{2}}\) exerted on the first rigid body by the second.
\(G\) is the gravitational constant (\(\frac{\text{m}^{3}}{\text{kg}\text{s}^{2}}\))
\({m_{1}}\) is the mass of the first body (\({\text{kg}}\))
\({m_{2}}\) is the mass of the second body (\({\text{kg}}\))
\(|\boldsymbol{d}|\) is the Euclidean norm of the distance between the center of mass of two bodies (\({\text{m}}\))
\(\boldsymbol{\hat{d}}\) is the unit vector directed from the center of the large mass to the center of the smaller mass (\({\text{m}}\))
\(\boldsymbol{d}\) is the distance between the center of mass of the rigid bodies (\({\text{m}}\))
Notes
Two rigid bodies in the universe attract each other with a force \(\boldsymbol{F}\) that is directly proportional to the product of their masses, \({m_{1}}\) and \({m_{2}}\), and inversely proportional to the squared distance \({|\boldsymbol{d}|^{2}}\) between them.
\(\boldsymbol{τ}\) is the torque (\(\text{N}\text{m}\))
\(\boldsymbol{I}\) is the moment of inertia (\(\text{kg}\text{m}^{2}\))
\(α\) is the angular acceleration (\(\frac{\text{rad}}{\text{s}^{2}}\))
Notes
The net torque \(\boldsymbol{τ}\) on a rigid body is proportional to its angular acceleration \(α\), where \(\boldsymbol{I}\) denotes the moment of inertia of the rigid body as the constant of proportionality.
We also assume that all rigid bodies involved are two-dimensional (from A:objectDimension).