For the quadratic Planck function profile,The optically thick limit and the instantaneous doubled-abundance result are thereforeThe new coefficient is β/4, since B(τ)=B0+β(τ/2)2 at fixed physical temperature. For positive β, the outgoing spectral irradiance decreases. The factor differs from the linear case because the temperature-dependent source function curves with depth; doubling abundance does not mean holding its old functional coefficients fixed in the new optical-depth coordinate.
I0=πB0+2πβ∫0τsτe−τdτ=πB0+2πβ[1−(1+τs)e−τs].
I0=π(B0+2β),I0=π(B0+β/2),ΔI0=−23πβ.
Ancestors (12)
- 3
- 1
- S25
- 2012
- Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
- Short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
- Physics course of the University of Oxford
- Undergraduate course of the University of Oxford
- Course of the University of Oxford
- University of Oxford
- List of universities
- Home
Discussion (0)
New discussionThere are no discussions about this article yet.
Articles by others on the same topic (0)
There are currently no matching articles.