courses:ast201:1
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| courses:ast201:1 [2023/10/02 00:33] – [5.1 Stellar aberration] asad | courses:ast201:1 [2023/10/02 00:45] (current) – [4. Newton and Einstein] asad | ||
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| Newton made gravity the physical reason behind planetary motions as opposed to Descartes' | Newton made gravity the physical reason behind planetary motions as opposed to Descartes' | ||
| - | $$ g = \frac{GM}{r^2} $$ | + | $$ \vec{g} = \frac{GM}{r^2} \hat{r} $$ |
| - | and the gravitational potential | + | where $G$ is the Newtonian gravitational constant, $M$ the mass of an object |
| $$ U = - \frac{GMm}{r} $$ | $$ U = - \frac{GMm}{r} $$ | ||
| for a small mass $m$ around a large mass $M$. | for a small mass $m$ around a large mass $M$. | ||
| + | |||
| + | The theory was later modified by Einstein as | ||
| + | |||
| + | $$ G_{\mu\nu} + \Lambda g_{\mu\nu} = \kappa T_{\mu\nu} $$ | ||
| + | |||
| + | where $G_{\mu\nu}$ is the [[bn: | ||
| + | |||
| + | $$ \kappa = \frac{8\pi G}{c^4} $$ | ||
| + | |||
| + | is the Einstein gravitational constant. | ||
| ===== - Stellar aberration and parallax ===== | ===== - Stellar aberration and parallax ===== | ||
| Line 84: | Line 94: | ||
| ==== - Stellar aberration ==== | ==== - Stellar aberration ==== | ||
| {{https:// | {{https:// | ||
| - | In this example of 2D frame moving only in the $x$-direction | + | |
| + | In this example of 2D frame moving only in the $x$-direction, the vertical component of the apparent speed of light ($u$) will not change, but the horizontal component will be modified due to the velocity of the Earth. | ||
| $$ \tan\phi = \frac{u_y' | $$ \tan\phi = \frac{u_y' | ||
| - | where $\gamma=(1-v^2/ | + | where $\gamma=(1-v^2/ |
| $$ \tan\phi = \frac{c\sin\theta}{\gamma(c\cos\theta+v)} = \frac{\sin\theta}{\gamma(v/ | $$ \tan\phi = \frac{c\sin\theta}{\gamma(c\cos\theta+v)} = \frac{\sin\theta}{\gamma(v/ | ||
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