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| 183_notes:grav_accel [2014/09/10 14:40] – [The Local Gravitational Acceleration revisited] caballero | 183_notes:grav_accel [2021/02/05 00:02] (current) – [The Gravitational Force and the Momentum Principle] stumptyl | ||
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| + | Section 3.2 and 3.3 in Matter and Interactions (4th edition) | ||
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| ===== Gravitational Acceleration ===== | ===== Gravitational Acceleration ===== | ||
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| $$\vec{a}_2 = -G\dfrac{m_1}{|\vec{r}|^2}\hat{r}$$ | $$\vec{a}_2 = -G\dfrac{m_1}{|\vec{r}|^2}\hat{r}$$ | ||
| - | The resulting expression is the acceleration that object 2 experiences due to it's gravitational interaction with object | + | // |
| - | So, in general: | + | So, __in general__: |
| $$\vec{a} = -G\dfrac{m}{|\vec{r}|^2}\hat{r}$$ | $$\vec{a} = -G\dfrac{m}{|\vec{r}|^2}\hat{r}$$ | ||
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| For simplicity, let's take the downward vertical direction to be positive. Let's compute the acceleration due gravity at the surface of the Earth. Here the [[http:// | For simplicity, let's take the downward vertical direction to be positive. Let's compute the acceleration due gravity at the surface of the Earth. Here the [[http:// | ||
| - | $$a_y=G\dfrac{M_{Earth}}{R_{Earth}} = \left(6.67384 \times 10^{-11} \dfrac{m^3}{kg\: | + | $$a_y=G\dfrac{M_{Earth}}{R^2_{Earth}} = \left(6.67384 \times 10^{-11} \dfrac{m^3}{kg\: |
| which is pretty close to the value we often use. In fact, the gravitational acceleration fluctuates a few percent over the surface of the Earth due to [[http:// | which is pretty close to the value we often use. In fact, the gravitational acceleration fluctuates a few percent over the surface of the Earth due to [[http:// | ||