angle of incidence = angle of reflection, both measured from the normal, in the plane of incidence
The angle of incidence equals the angle of reflection, both measured from the normal, and the incident ray, reflected ray and normal lie in one plane.
The two laws of reflection for any reflecting surface.
- angle of incidence
- angle between incident ray and normal (degree)
- angle of reflection
- angle between reflected ray and normal (degree)
Use when — Any reflecting boundary, plane or curved, at the point of incidence.
Common trap — Measuring the angle from the surface instead of from the normal.
1/v + 1/u = 1/f
One over image distance plus one over object distance equals one over focal length, all measured with a fixed sign convention.
Relates object distance, image distance and focal length for a spherical mirror.
- u
- object distance from the pole, with sign convention (m)
- v
- image distance from the pole, with sign convention (m)
- f
- focal length, with sign convention (m)
Use when — A spherical mirror problem after a sign convention has been fixed and a ray diagram drawn.
Common trap — Mixing signs from two different conventions within the same solution.
f = R / 2
Focal length equals half the radius of curvature.
Relates the focal length of a spherical mirror to its radius of curvature.
- f
- focal length (m)
- R
- radius of curvature (m)
Use when — A spherical mirror problem where the radius of curvature is given instead of the focal length.
Common trap — Applying this relation to a lens instead of a mirror.
m = -v/u
Magnification equals minus image distance divided by object distance.
Magnification produced by a spherical mirror.
- m
- magnification, ratio of image height to object height with sign (no unit)
Use when — Comparing image size and orientation to the object for a mirror.
Common trap — Dropping the negative sign and losing the inversion information.
n1 sin(theta1) = n2 sin(theta2)
The refractive index of the first medium times the sine of the angle of incidence equals the refractive index of the second medium times the sine of the angle of refraction.
Refraction of a ray crossing a plane boundary between two media.
- n1, n2
- refractive indices of the two media (no unit)
- theta1, theta2
- angles of incidence and refraction from the normal (degree)
Use when — A ray crosses a plane refracting boundary.
Common trap — Swapping which medium's index multiplies which angle.
n2/v - n1/u = (n2 - n1) / R
The second index over image distance minus the first index over object distance equals the difference of the two indices over the radius of curvature.
Refraction at a single spherical surface separating two media.
- n1
- refractive index of the medium containing the incident ray (no unit)
- n2
- refractive index of the medium containing the refracted ray (no unit)
- u
- object distance from the surface, with sign convention (m)
- v
- image distance from the surface, with sign convention (m)
- R
- radius of curvature of the surface, with sign convention (m)
Use when — A single curved refracting surface, as the building block behind the lens maker relation.
Common trap — Using the wrong index on the wrong side of the equation.
sin(theta_c) = n2/n1, with n1 > n2; total internal reflection when theta1 > theta_c
The sine of the critical angle equals the ratio of the rarer to the denser refractive index; total internal reflection occurs only when the angle of incidence exceeds this critical angle, travelling from denser to rarer medium.
Condition for total internal reflection at a boundary from a denser to a rarer medium.
- theta_c
- critical angle (degree)
- n1
- refractive index of the denser medium (no unit)
- n2
- refractive index of the rarer medium (no unit)
Use when — Light travels from a denser medium toward a rarer medium and the angle of incidence must be checked against the critical angle.
Common trap — Checking the angle condition without also checking that the ray goes from denser to rarer medium.
1/v - 1/u = 1/f
One over image distance minus one over object distance equals one over focal length, all measured with a fixed sign convention.
Relates object distance, image distance and focal length for a thin lens.
- u
- object distance from the optical centre, with sign convention (m)
- v
- image distance from the optical centre, with sign convention (m)
- f
- focal length, with sign convention (m)
Use when — A thin lens problem after a sign convention has been fixed.
Common trap — Using the mirror-formula sign pattern for a lens or vice versa.
1/f = (n_lens/n_medium - 1) (1/R1 - 1/R2)
The reciprocal of focal length equals the ratio of lens index to medium index minus one, multiplied by the difference of the reciprocals of the two radii of curvature.
Gives the focal length of a thin lens from its material, surrounding medium and surface curvatures.
- n_lens
- refractive index of the lens material (no unit)
- n_medium
- refractive index of the surrounding medium (no unit)
- R1, R2
- radii of curvature of the first and second lens surfaces, with sign convention (m)
Use when — The lens geometry and material indices are given, under the thin-lens approximation.
Common trap — Assigning R1 and R2 signs inconsistently with the direction of light travel.
m = v/u ; P = 1/f (f in metres)
Lens magnification equals image distance divided by object distance; power equals one over focal length in metres, measured in dioptres.
Magnification of a thin lens and the definition of lens power.
- m
- magnification (no unit)
- P
- power of a lens (dioptre)
Use when — Comparing image size to object size for a lens, or combining lens powers.
Common trap — Confusing the sign convention for lens magnification with the mirror magnification convention.
1/F = 1/f1 + 1/f2 + ... ; P = P1 + P2 + ...
The reciprocal of the combined focal length equals the sum of the reciprocals of the individual focal lengths; combined power equals the sum of individual powers.
Effective focal length and power of thin lenses placed in contact.
- F
- effective focal length of the combination (m)
- f1, f2
- focal lengths of individual lenses (m)
Use when — Multiple thin lenses are in contact along a common axis.
Common trap — Applying this direct sum to lenses that are separated by a finite distance instead of in contact.
delta = (theta_i + theta_e) - A ; at minimum deviation, n = sin((A + delta_m)/2) / sin(A/2)
Deviation equals the sum of the incidence and emergence angles minus the prism angle; at minimum deviation, refractive index equals the sine of half the sum of prism angle and minimum deviation, divided by the sine of half the prism angle.
Angle of deviation produced by a prism, and the refractive index formula at minimum deviation.
- delta
- angle of deviation (degree)
- theta_i
- angle of incidence (degree)
- theta_e
- angle of emergence (degree)
- A
- prism (refracting) angle (degree)
- delta_m
- minimum deviation, occurring at one specific angle of incidence (degree)
Use when — The general deviation relation applies to any angle of incidence; the minimum-deviation index formula applies only at that specific minimum-deviation condition.
Common trap — Using the minimum-deviation index formula when the angle of incidence is not actually the minimum-deviation angle.