Integrating Over All Orientations: Solving Eqn (1)

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SUMMARY

The discussion centers on integrating over solid angles in the context of scattering events, specifically solving the equation \(\int d\Omega_1 d\Omega_2 d\Omega_3\). The integration over a single solid angle yields \(4\pi\), leading to the conclusion that integrating three solid angles results in \(64\pi^3\). The participants clarify that each particle can have its own orientation, which is crucial for calculating the density of states, represented as \(d^9 n \propto p_e p_\nu1 p_\nu2 dp_e dp_\nu d\Omega_e d\Omega_1 d\Omega_2\).

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physguy09
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So I need to inegrate over a solid angle, in which every possible orientation is considered (we are doing scattering events in which we assume every possible angle is possible), thus I need to solve
\int d\Omega_1 d\Omega_2 d\Omega_3 Eqn (1).

Now I know

\int^{2 \pi}_{0} \int^{\pi}_{0}d\Omega = \int^{2 \pi}_{0} \int^{\pi}_{0} sin(\theta)d\theta d\phi = 2\pi \int^{\pi}_{0} sin(\theta) d\theta = 2\pi (-cos(\theta))^{\pi}_{0} = 4 \pi
so shouldn't that mean that Eqn (1) should integrate to 64 \pi^3?
 
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Hi physguy09! :smile:

(have an omega: Ω :wink:)
physguy09 said:
\int d\Omega_1 d\Omega_2 d\Omega_3 Eqn (1).

I don't understand … how can you have more than one Ω? (more than one solid angle?) :confused:
 
the original problem asks us to calculate the density of states
d^9 n \propto p_e p_\nu1 p_\nu2 dp_e dp_\nu d\Omega_e d\Omega_1 d\Omega_2
where each individual particle is allowed to undergo its own possible orientation independent of the other particles (as there is no attraction amongst these, since we have two neutrinos and an e-.
 

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