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courses:ast201:1 [2023/10/02 00:33] – [5.1 Stellar aberration] asadcourses: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' mysterious vortices. The full form his gravitational acceleration Newton made gravity the physical reason behind planetary motions as opposed to Descartes' mysterious vortices. The full form his gravitational acceleration
  
-$$ g = \frac{GM}{r^2} $$+$$ \vec{g= \frac{GM}{r^2} \hat{r} $$
  
-and the gravitational potential+where $G$ is the Newtonian gravitational constant, $M$ the mass of an object and $r$ is the distance at which the acceleration is being calculated. This $\vec{g}$ can be thought of also as a gravitational field around a massive object. The gravitational potential
  
 $$ U = - \frac{GMm}{r} $$ $$ U = - \frac{GMm}{r} $$
  
 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:Einstein tensor]], $g_{\mu\nu}$ is the metric tensor, $T_{\mu\nu}$ is the stress-energy tensor, $\Lambda$ is the cosmological constant and 
 +
 +$$ \kappa = \frac{8\pi G}{c^4} $$
 +
 +is the Einstein gravitational constant.
  
 ===== - Stellar aberration and parallax ===== ===== - Stellar aberration and parallax =====
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 ==== - Stellar aberration ==== ==== - Stellar aberration ====
 {{https://upload.wikimedia.org/wikipedia/commons/9/93/Simple_stellar_aberration_diagram.svg?nolink}} {{https://upload.wikimedia.org/wikipedia/commons/9/93/Simple_stellar_aberration_diagram.svg?nolink}}
-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.
  
 $$ \tan\phi = \frac{u_y'}{u_x'} = \frac{u_y}{\gamma(u_x+v)} $$ $$ \tan\phi = \frac{u_y'}{u_x'} = \frac{u_y}{\gamma(u_x+v)} $$
  
-where $\gamma=(1-v^2/c^2)^{-1/2}$ and $v$ is the velocity of the observer. The velocity components of light in the rest and moving frame are $(u_x,u_y)$ and $(u_x',u_y')$, respectively and $c^2 = u_x^2 + u_y^2$. So+where $\gamma=(1-v^2/c^2)^{-1/2}$$v$ is the velocity of the observer and $c$ is the magnitude of the velocity of light. The velocity components of light in the rest and moving frames are $(u_x,u_y)$ and $(u_x',u_y')$, respectively and $c^2 = u_x^2 + u_y^2$. So
  
 $$ \tan\phi = \frac{c\sin\theta}{\gamma(c\cos\theta+v)} = \frac{\sin\theta}{\gamma(v/c+\cos\theta)}. $$ $$ \tan\phi = \frac{c\sin\theta}{\gamma(c\cos\theta+v)} = \frac{\sin\theta}{\gamma(v/c+\cos\theta)}. $$
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