Respuesta :
Let's do it algebraically by first defining some variables. Use SI units.
Radius of the planet: [tex] r_{0} [/tex]
Distance between the spacecraft and the center of the planet: [tex] r_{1} = r_{0} + 14000000[/tex]
Mass of the planet: [tex]M[/tex]
Mass of the spacecraft: [tex]m[/tex]
Tangential velocity of the spacecraft in its orbit: [tex]v[/tex]
Angular velocity of the spacecraft: [tex]w= \frac{v}{ r_{1} } [/tex]
Orbital period of the spacecraft: [tex]T = \frac{2 \pi }{w} [/tex]
Since the centripetal force acting on the spacecraft is the gravitational force from the planet at distance [tex] r_{1} [/tex] from the planet's centre:
[tex] F_{c} = F_{g} ;\\ m \frac{v^{2}}{ r_{1} } = G \frac{mM}{r_{1}^{2} }[/tex]
Note we can cancel out the mass of the spacecraft.
Using the formula in the definitions above, substitute:
[tex] \frac{v^{2} }{r_{1} } = w^2 r_{1} = \frac{4 \pi^2 }{T^2} r_{1} [/tex]
So we can substitute for this expression and obtain
[tex] \frac{4 \pi ^2}{T^2} r_{1} =G \frac{M}{ r_{1}^2 } ; \\ M = \frac{4 \pi ^2 r_{1}^3 }{T^2 G} [/tex]
So now that we have the mass of the planet, we can easily calculate that [tex]g[/tex], the acceleration due to gravity on its surface, is given by:
[tex]g=G \frac{M}{ r_{0}^2 } = \frac{G}{ r_{0}^2 } \frac{4 \pi ^2 r_{1}^3 }{T^2G} = \frac{4 \pi ^2 r_{1}^3 }{ r_{0}^2 T^2 }[/tex]
Radius of the planet: [tex] r_{0} [/tex]
Distance between the spacecraft and the center of the planet: [tex] r_{1} = r_{0} + 14000000[/tex]
Mass of the planet: [tex]M[/tex]
Mass of the spacecraft: [tex]m[/tex]
Tangential velocity of the spacecraft in its orbit: [tex]v[/tex]
Angular velocity of the spacecraft: [tex]w= \frac{v}{ r_{1} } [/tex]
Orbital period of the spacecraft: [tex]T = \frac{2 \pi }{w} [/tex]
Since the centripetal force acting on the spacecraft is the gravitational force from the planet at distance [tex] r_{1} [/tex] from the planet's centre:
[tex] F_{c} = F_{g} ;\\ m \frac{v^{2}}{ r_{1} } = G \frac{mM}{r_{1}^{2} }[/tex]
Note we can cancel out the mass of the spacecraft.
Using the formula in the definitions above, substitute:
[tex] \frac{v^{2} }{r_{1} } = w^2 r_{1} = \frac{4 \pi^2 }{T^2} r_{1} [/tex]
So we can substitute for this expression and obtain
[tex] \frac{4 \pi ^2}{T^2} r_{1} =G \frac{M}{ r_{1}^2 } ; \\ M = \frac{4 \pi ^2 r_{1}^3 }{T^2 G} [/tex]
So now that we have the mass of the planet, we can easily calculate that [tex]g[/tex], the acceleration due to gravity on its surface, is given by:
[tex]g=G \frac{M}{ r_{0}^2 } = \frac{G}{ r_{0}^2 } \frac{4 \pi ^2 r_{1}^3 }{T^2G} = \frac{4 \pi ^2 r_{1}^3 }{ r_{0}^2 T^2 }[/tex]