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Purdue ME 606: Reflection from Surfaces

Specular reflection from ideal surfaces

θi = θr

dωi = dωr

Occurs for flat clean surfaces

σ= Standard deviation of surface height

For a surface to be smooth

\frac{\sigma }{\lambda } \ll 1

Diffuse Reflection

Ir=constant


\frac{\sigma }{\lambda } \gg 1

Real surface Reflection

Near-normal incident angles

-Approach above limits

-Superposition is possible

Large incident angles

-Diffuses approximately breaks down

-Forward scattering observed

Reflectance

Specular reflectance

θi = θr

\rho _s(\theta _i )=\frac{{I_r (\theta _r =\theta _i )}}{{I_i (\theta _i )}}

Reflection from non-metals

\rho _{s \bot }=\frac{{\tan ^2 (\theta _1  - \theta _2 )}}{{\tan ^2 (\theta _1  + \theta _2 )}}

\rho _{s\parallel }=\frac{{\sin ^2 (\theta _1  - \theta _2 )}}{{\sin ^2 (\theta _1  + \theta _2 )}}

Relate with Snell’s Law


sin(θ1) = n21sin(θ2)

n_{21}=\frac{{n_2 }}{{n_1 }}

= Index of refraction

\rho _s  = \frac{1}{2}(\rho _{s \bot }  + \rho _{s\parallel } )

For metals

Considering waves from vacuum (n=1)

n_{21}=\frac{{n_2 }}{{n_1 }}

n2 = n

For normal incidence

\rho _\parallel   = \rho _ \bot   = \frac{{(n - 1)^2  + \kappa^2 }}{{(n - 1)^2  + \kappa^2 }}

    • check this equation


for θi = 0

κ=Absorption coefficient

More algebraic complication for non-normal angles of incidence

Last modified on 14 Dec, 2008