B Gravitational field strength calculation

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The discussion clarifies when to use the equations g = F/m and g = GM/r² for calculating gravitational field strength. The equation g = F/m is used to determine the gravitational force acting on a mass in a gravitational field, while g = GM/r² calculates the field strength at a specific point created by a mass M. The latter is applicable for distances from a point mass or outside a spherically symmetric mass distribution. At the Earth's surface, g = GM/R² is used, with R being the Earth's radius, while at greater distances, r replaces R in the equation. Understanding these distinctions is crucial for accurate gravitational calculations.
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In what scenarios would you use the equation g= F/m instead of g=GM/r2 (or vice versa), for calculating gravitational field strength?

Update: is g=F/m used to find the force acting on a mass in a gravitational field (of strength g), whereas g=GM/r2 used to calculate the gravitational field strength at a point in the field created by the object of mass M
 
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g = F/m defines the strength of the gravitational field at any location, in terms of the gravitational force F that acts on a test-mass m placed at that location. (Note that we use a similar definition for electric field: E = Felectric/q.)

g = GM/r2 is an application of that definition to the special case of the gravitational field at a distance r from a point mass, or outside a spherically symmetric mass distribution, at a distance r from the center: $$g = \frac F m = \frac {\left( \frac {GMm} {r^2} \right)} m = \frac {GM} {r^2}$$
 
jtbell said:
g = F/m defines the strength of the gravitational field at any location, in terms of the gravitational force F that acts on a test-mass m placed at that location. (Note that we use a similar definition for electric field: E = Felectric/q.)

g = GM/r2 is an application of that definition to the special case of the gravitational field at a distance r from a point mass, or outside a spherically symmetric mass distribution, at a distance r from the center: $$g = \frac F m = \frac {\left( \frac {GMm} {r^2} \right)} m = \frac {GM} {r^2}$$

Ahh I see that makes sense, thank you
 
Maybe this is what you are asking since you are using lower case g... The gravitational force on a test mass m at a distance r from the center of the Earth is given by GmM/r2, where M is the mass of the earth. At the Earth's surface, the force is given by GmM/R2, where R is the radius of the earth. For small distances from the surface, this equation still holds well and we use g = GM/R2 for the acceleration due to gravity near the Earth's surface, in which case F=mg.

At appreciable distances from the Earth's surface, we have to use r instead of R, hence the other equation.
 
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