Figure 1: Portrait of Isaac Newton (by courtesy of SEDS).
Two bodies attract each other with equal and opposite forces; the magnitude of this force is proportional to the product of the two masses and is also proportional to the inverse square of the distance between the centers of mass of the two bodies.
F = G . M . m / r^{2}
where m and M are the masses of the two bodies, r is the distance between the two, and G is the gravitational constant, whose value is :
G = 6.67 . 10^{-11} Newton.metre^{2}/kg^{2}
The force with which the Earth attracts bodies situated near to its surface is called body's weight.
The weight of a mass m, located on the Earth's surface is :
P = m . g
This expression is an immediate consequence of the Universal Gravitation Law and of Newton's Second Law.
Under normal conditions, the value of g is approximately equal to 9.8 metres/second ^{2}.
According to Newton's Third Law, if a body acts on another with a certain force, the latter one acts on the former with an equivalent force in opposite direction. This happens with the Universal Gravitation Law, where the force that a body with mass M exerts on another body of mass m is the same as that exerted by the body of mass m on the body of mass M (although in opposite direction). However, although these forces are equal, the accelerations are not. By applying Newton's Second Law we will have:
Considering that acceleration is the second derivative with respect to time, we have that the acceleration of a body subject to the gravitational action of another body of mass M is:
d^{2}r/dt^{2} = G . M / r^{2}
We use a cartesian co-ordinates permanently situated in the center of the body with mass M. For this reason, the position of the body of mass m coincides with its distance r to the origin of co-ordinates (its radius vector).
Changing the previous equation to cartesian co-ordinates (x,y) we obtain:
d^{2}x/dt^{2} = G . M . x / r^{3}
d^{2}y/dt^{2} = G . M . y / r^{3}
where r = square root (x^{2} + y^{2}) Depending on the masses of the two bodies, and the initial conditions (the initial positions and velocities) the trajectory of the moving body may be:
Last modified 21/12/99 by Juan de Lara ( Juan.Lara@ii.uam.es, http://www.ii.uam.es/~jlara) need help for using this courses?.