The acceleration due to gravity at the Earth's surface depends on
both its mass and radius.
The acceleration due to gravity, often denoted by 'g', is a fundamental concept in physics. It represents the acceleration experienced by an object falling freely near the surface of a massive body like the Earth, assuming no air resistance. The value of this acceleration is not constant throughout the universe; it depends on the properties of the massive body itself.
The acceleration due to gravity (g) on the surface of a planet can be calculated using Newton's Law of Universal Gravitation. The formula is given by:
Let's break down what each term in this formula represents:
Looking at the formula \(g = \frac{GM}{R^2}\), we can clearly see which physical properties of the Earth influence the value of 'g' at its surface:
Therefore, the acceleration due to gravity at the Earth's surface is determined by the combined values of Earth's mass (\(M\)) and Earth's radius (\(R\)).
| Factor | Influence on 'g' | Notes |
|---|---|---|
| Earth's Mass (\(M\)) | Directly proportional | Higher mass means higher 'g' |
| Earth's Radius (\(R\)) | Inversely proportional to \(R^2\) | Higher radius means lower 'g' |
| Gravitational Constant (\(G\)) | Constant factor | Universal value |
Based on the analysis of the formula and the factors involved, the acceleration due to gravity at the Earth's surface depends on both its mass and its radius.
| Concept | Formula Relation | Key Dependency |
|---|---|---|
| Acceleration due to gravity (g) | \(g \propto M\) | Planet's Mass |
| Acceleration due to gravity (g) | \(g \propto \frac{1}{R^2}\) | Planet's Radius |
While the formula \(g = \frac{GM}{R^2}\) gives the theoretical value of acceleration due to gravity at the surface, the actual value varies slightly across the Earth's surface. These variations are due to:
However, the primary factors determining the average acceleration due to gravity at the Earth's surface are still its total mass and average radius, as described by the formula.
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D. The orbit of a planet is circular with another planet in the center.
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