n1 sin i = n2 sin r
n one sine i equals n two sine r, with both angles measured from the normal.
Snell's law of refraction at a boundary between isotropic media.
- n1, n2
- refractive indices of the two media (dimensionless)
- i
- angle of incidence, measured from the normal
- r
- angle of refraction, measured from the normal
Use when — Refraction at a boundary between isotropic media.
Common trap — Measuring angles from the surface instead of the normal.
sin c = n2 / n1
Sine of the critical angle equals n two over n one, with n one the denser medium.
The critical angle for total internal reflection.
- c
- critical angle
- n1, n2
- refractive indices, with n1 greater than n2 (dimensionless)
Use when — Ray travels from a denser optical medium to a rarer one.
Common trap — Using the relation in the opposite direction of travel.
1/f = 1/v + 1/u
One over f equals one over v plus one over u, all signed under one convention.
Spherical mirror relation between object distance, image distance and focal length.
- f
- focal length (m)
- u
- object distance (m)
- v
- image distance (m)
Use when — Paraxial spherical mirror with one fixed sign convention.
Common trap — Substituting unsigned distances.
1/f = 1/v - 1/u
One over f equals one over v minus one over u.
Thin-lens relation between object distance, image distance and focal length.
- f
- focal length (m)
- u
- object distance (m)
- v
- image distance (m)
Use when — Paraxial thin lens.
Common trap — Mixing the mirror and lens sign forms.
m = -v/u for a mirror ; m = v/u for a lens
Magnification is minus v over u for a mirror, and v over u for a lens.
Lateral magnification of the image relative to the object.
- m
- lateral magnification (dimensionless)
- u, v
- object and image distances under the same sign convention (m)
Use when — Same sign convention as the imaging formula in use.
Common trap — Reading magnitude only and losing image orientation.
1/f = (n - 1) (1/R1 - 1/R2)
One over f equals n minus one, times the difference of one over R one and one over R two.
Lens maker relation for a thin lens in air.
- f
- focal length (m)
- n
- refractive index of the lens material relative to air (dimensionless)
- R1, R2
- radii of curvature of the two surfaces (m)
Use when — Thin lens in air with stated surface signs.
Common trap — Using it unchanged when the lens sits in another surrounding medium.
n = sin[(A + delta_m) / 2] / sin(A / 2)
n equals sine of half the sum of A and delta m, divided by sine of half A.
Refractive index of a prism at the symmetric minimum-deviation path.
- A
- prism angle
- delta_m
- angle of minimum deviation
- n
- refractive index of the prism material (dimensionless)
Use when — Homogeneous prism at the symmetric minimum-deviation path where i = e and r1 = r2 = A/2.
Common trap — Using a general deviation value in place of delta_m.
beta = lambda D / d
Fringe width beta equals lambda D over d.
Fringe width in Young's double slit experiment.
- beta
- fringe width (m)
- lambda
- wavelength of light (m)
- D
- screen distance from the slits (m)
- d
- slit separation (m)
Use when — Small-angle geometry, coherent sources, and D much greater than d.
Common trap — Confusing slit separation d with slit width.
a sin(theta) = m lambda
a sine theta equals m lambda, for m equal to one, two, three and so on.
Angular position of minima in single-slit diffraction.
- a
- slit width (m)
- lambda
- wavelength of light (m)
- theta
- angle from the central axis
- m
- minimum order, m = 1, 2, 3 ...
Use when — Fraunhofer single-slit diffraction.
Common trap — Treating m = 0 as a minimum.
tan(i_B) = n2 / n1
Tangent of the Brewster angle equals n two over n one.
Brewster's angle, at which reflected light is plane-polarized.
- i_B
- Brewster angle
- n1, n2
- refractive indices of the incident and second medium (dimensionless)
Use when — Reflected light is plane-polarized at Brewster incidence.
Common trap — Assuming the reflected and refracted rays are unrelated at this condition.