Math 2.0

Astronomy and astrophysics Definition

Limb darkening

Builds on Optical depth

Definition

Consider a spherical star seen from far away. For a point on its visible disk, let θ\theta be the angle between the line of sight and the outward normal to the surface there. Let μ=cos⁡θ∈[0,1]\mu = \cos\theta \in [0, 1]. Let I(μ)I(\mu) be the specific intensity of the emergent radiation in the direction of the observer. The star shows limb darkening when I(μ)I(\mu) is an increasing function of μ\mu, so that I(μ)<I(1)I(\mu) < I(1) for μ<1\mu < 1; the ratio I(μ)/I(1)I(\mu)/I(1) is the limb-darkening law.

Remarks

Example: in a grey atmosphere in the Eddington approximation, the source function is linear in the optical depth, S(τ)=a+bτS(\tau) = a + b\tau with b=3a/2>0b = 3a/2 > 0. The emergent intensity is then I(μ)=a+bμI(\mu) = a + b\mu, so I(μ)/I(1)=(2+3μ)/5I(\mu)/I(1) = (2 + 3\mu)/5. This increases with μ\mu and equals 2/52/5 at the limb. Non-example: a semi-infinite atmosphere with constant source function SS gives I(μ)=SI(\mu) = S for all μ\mu, so there is no limb darkening. A common empirical form is the linear law I(μ)/I(1)=1−u(1−μ)I(\mu)/I(1) = 1 - u(1 - \mu) with a coefficient uu that depends on wavelength. The Eddington–Barbier relation I(μ)≈S(τ=μ)I(\mu) \approx S(\tau = \mu) explains the effect: the observer sees down to optical depth about μ\mu along the normal.

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  1. Optical depth concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Limb_darkening
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MSC85A25, 85A15
DefinesLimb darkening
UsesOptical depth
Changed3 November 2026

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