Physics:Effective radius
The effective radius or half-light radius ([math]\displaystyle{ R_e }[/math]) of a galaxy is the radius at which half of the total light of the system is emitted.[1][2] This assumes the galaxy has either intrinsic spherical symmetry or is at least circularly symmetric as viewed in the plane of the sky. Alternatively, a half-light contour, or isophote, may be used for spherically and circularly asymmetric objects.
[math]\displaystyle{ R_e }[/math] is an important length scale in [math]\displaystyle{ \sqrt[4] R }[/math] term in de Vaucouleurs law,[3] which characterizes a specific rate at which surface brightness decreases as a function of radius:
- [math]\displaystyle{ I(R) = I_e \cdot e^{-7.67 \left( \sqrt[4]{\frac R {R_e}} - 1 \right)} }[/math]
where [math]\displaystyle{ I_e }[/math] is the surface brightness at [math]\displaystyle{ R = R_e }[/math]. At [math]\displaystyle{ R = 0 }[/math],
- [math]\displaystyle{ I(R=0) = I_e \cdot e^{7.67} \approx 2000 \cdot I_e }[/math]
Thus, the central surface brightness is approximately [math]\displaystyle{ 2000 \cdot I_e }[/math].
See also
References
- ↑ "Half-light Radius". Swinburne University. http://astronomy.swin.edu.au/cms/astro/cosmos/h/Half-light+Radius. Retrieved 22 May 2013.
- ↑ Binney, James; Tremaine, Scott (2008). Galactic Dynamics (Second ed.). Princeton Series in Astrophysics. p. 21. ISBN 9780691130279.
- ↑ Mazure, Alain (15 February 2002). "Exact solutions for the spatial de Vaucouleurs and Sérsic laws and related quantities". Astronomy & Astrophysics 383 (2): 384–389. doi:10.1051/0004-6361:20011751. Bibcode: 2002A&A...383..384M. https://www.aanda.org/articles/aa/pdf/2002/08/aa1928.pdf.