The centre of mass of an extended body on the surface of the earth and its centre of gravity
The center of mass and the center of gravity are related concepts but have key differences:
Center of Mass:
Center of Gravity:
In summary: The center of mass is related to mass distribution, while the center of gravity is related to the distribution of the gravitational force. In most practical situations where gravity is uniform, the two points coincide.
Let's define the Center of Mass (CM) and Center of Gravity (CG) for an extended body.
The CM and CG coincide if and only if the gravitational field \( \vec{g} \) is uniform across the entire extent of the body. If \( \vec{g} \) is constant (same magnitude and direction for all particles \( i \)), then \( \vec{g}_i = \vec{g} \) for all \( i \), and the formula for CG simplifies: \[ \vec{r}_{CG} = \frac{\sum m_i \vec{g} \times \vec{r}_i}{\sum m_i \vec{g}} = \frac{\vec{g} \sum m_i \vec{r}_i}{\vec{g} \sum m_i} = \frac{\sum m_i \vec{r}_i}{\sum m_i} = \vec{r}_{CM} \]
Now consider an extended body on the surface of the Earth. The Earth's gravitational field is not perfectly uniform. The magnitude of \( \vec{g} \) decreases with altitude (distance from the Earth's center), and its direction always points towards the Earth's center. For a large extended body (e.g., a very tall building or a mountain), the gravitational field at the top of the body will be slightly weaker and point in a slightly different direction compared to the field at the bottom.
However, if the size of the body is negligible compared to the radius of the Earth (which is approximately 6400 km), the variation in the gravitational field \( \vec{g} \) across the body is extremely small and can be ignored. In this common scenario, we can approximate the gravitational field as uniform over the body.
Therefore:
Evaluating the options:
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