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Assisted-by: GLM 5.3
930 B
930 B
Math
Inline radiation: E = h\nu redshifted by \sqrt{g_{tt}}.
E = h\nu\,\sqrt{g_{tt}(r)} = \text{konst.} \quad (1)
The metric reads ds^2 = -g_{tt}(r)c^2dt^2 + dr^2 + r^2d\Omega^2, and a
photon loses energy as \frac{E(t)}{E_0} = e^{-Ht}.
1+z = \frac{\nu(r_1)}{\nu(r_2)} = \sqrt{\frac{g_{tt}(r_1)}{g_{tt}(r_2)}}. \quad (2)
Prices are not math: the ticket costs $5 and the guide $10 per group.
The metric in prose right above its display form
g_{tt}(r) = 1 - \frac{r_s}{r}
continues in a sentence after it.
$$r_h = \frac{\sigma}{\sqrt{2\pi G \rho_{\text{amb}}}}, \qquad M_h = \frac{2\sigma^2 r_h}{G}. \quad (7)$$
An equation broken across lines keeps its prose out of mathematics
$\nabla^2 h =
(8\pi/\kappa a)u$: the binding is the force of a cell \kappa a = c^4/G,
and the source is the energy.
\raisebox{1em}{E} = h\nu
Inline degradation too: \raisebox{1em}{E} stays visible where it stands.