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Refraction of Light at Plane Surfaces — Notes

6 sections 6 min readBeta

1. Refraction and its laws

  • Refraction: the change in direction of light as it passes obliquely from one transparent medium into another. Cause: light has different speeds in different media.
  • At every boundary there is also partial reflection (a faint reflection in a window pane).
  • Rarer → denser: ray bends towards the normal; denser → rarer: away from the normal.
  • Laws of refraction: (1) incident ray, refracted ray and normal at the point of incidence lie in one plane; (2) Snell’s law — sin⁡i/sin⁡r\sin i / \sin r is constant for a given pair of media and a given colour.
  • On entering a denser medium: speed and wavelength decrease, frequency (and so colour) is unchanged.
  • No deviation when (i) i=0i = 0 (along the normal) or (ii) both media have the same refractive index.
Table of the changes in light on entering a denser medium
Into a denser mediumChange
SpeedDecreases
WavelengthDecreases
FrequencyUnchanged
Direction (oblique ray)Bends towards the normal

Formulas

  • Snell’s law
    sin⁡isin⁡r=1μ2\frac{\sin i}{\sin r} = {}_{1}\mu_{2}
  • Wave equation
    v=fλv = f \lambda

Key terms

Refraction

Bending of light when it passes obliquely from one transparent medium into another, because its speed changes.

Snell’s law

For a given pair of media and colour of light, the sine of the angle of incidence divided by the sine of the angle of refraction is a constant.

2. Refractive index

  • Absolute refractive index: μ=c/v\mu = c / v, with c=3×108c = 3 \times 10^{8} m s⁻¹. No unit; greater than 1 for every material medium.
  • Larger μ\mu → slower light → optically denser (optical density is not the same as mass density: kerosene is optically denser than water but floats on it).
  • Relative refractive index:  1μ2=μ2/μ1=v1/v2\,{}_{1}\mu_{2} = \mu_{2} / \mu_{1} = v_{1} / v_{2}.
  • μ\mu depends on the material, the colour (wavelength) of light (larger for violet than red) and slightly on temperature.
  • Typical values: water 1.33, glass 1.5, diamond 2.42.
Table of refractive indices and speeds of light in three media
MediumμSpeed (× 10⁸ m/s)
Water1.332.25
Glass1.52.0
Diamond2.421.24

Formulas

  • Refractive index from speeds
    μ=cv\mu = \frac{c}{v}
  • Relative refractive index
    1μ2=μ2μ1=v1v2{}_{1}\mu_{2} = \frac{\mu_{2}}{\mu_{1}} = \frac{v_{1}}{v_{2}}

Key terms

Absolute refractive index

Ratio of the speed of light in vacuum to the speed of light in the medium.

Optically denser medium

A medium with a larger refractive index, in which light travels more slowly.

3. Rectangular glass block and thick mirror

  • Ray bends towards the normal at the first face and away at the second; the faces are parallel, so e = i and the emergent ray is parallel to the incident ray.
  • Lateral displacement: perpendicular distance between the incident ray produced and the emergent ray. It increases with the thickness of the block, the angle of incidence and the refractive index; it is zero for normal incidence.
  • Thick plane mirror (silvered at the back): partial reflection at the front glass surface gives a faint first image; reflection at the silvered back gives the brightest (second) image; repeated internal reflections give further, fainter images. All emergent rays are parallel.
Table of the images formed by a thick plane mirror
Image in a thick mirrorFormed byBrightness
FirstReflection at the front glass surfaceFaint
SecondReflection at the silvered backBrightest
Third and laterRepeated internal reflectionFainter and fainter

Formulas

  • Parallel-sided block
    e=ie = i

Key terms

Lateral displacement

The perpendicular distance between the incident ray produced and the emergent ray of a parallel-sided block.

Angle of emergence

The angle between the emergent ray and the normal at the second face.

4. Real and apparent depth

  • Rays from an object under water bend away from the normal on leaving; produced back they meet above the object, which appears raised.
  • For near-normal viewing: μ=real depthapparent depth\mu = \dfrac{\text{real depth}}{\text{apparent depth}}.
  • Shift (apparent rise) =real depth−apparent depth=real depth (1−1/μ)= \text{real depth} - \text{apparent depth} = \text{real depth}\,(1 - 1/\mu).
  • Viewed obliquely, the object appears raised even more.
  • Effects: a pool looks shallower; a stick dipped obliquely looks bent at the surface; print under a glass block looks raised; to a fish, a bird looks higher.
Table of real depth, refractive index, apparent depth and shift for three cases
Real depthμApparent depthShift
12 cm4/39 cm3 cm
9 cm1.56 cm3 cm
5 m1.254 m1 m

Formulas

  • Real and apparent depth
    μ=real depthapparent depth\mu = \frac{\text{real depth}}{\text{apparent depth}}
  • Apparent rise for real depth d
    shift=d(1−1μ)\text{shift} = d\left(1 - \frac{1}{\mu}\right)

Key terms

Apparent depth

The depth at which an object in a denser medium appears to be when viewed from the rarer medium.

Shift

The distance by which an object under a denser medium appears raised: real depth minus apparent depth.

5. Refraction through a triangular prism

  • A prism has two refracting faces inclined at the angle of the prism AA.
  • The ray bends towards the normal at the first face and away from it at the second; the emergent ray is turned towards the base.
  • Angle of deviation δ\delta: angle between the incident ray produced and the emergent ray.
  • Relations: r1+r2=Ar_{1} + r_{2} = A; δ=i+e−A\delta = i + e - A.
  • δ\delta depends on (i) angle of incidence, (ii) angle of the prism, (iii) refractive index of the material, (iv) colour of light (violet deviates most). As ii increases, δ\delta first decreases to a minimum, then increases.
Table of factors that change the angle of deviation of a prism
ChangeEffect on deviation
Larger prism angle ALarger
Larger refractive indexLarger
Violet light instead of redLarger
Angle of incidence increasedFirst less, then more

Formulas

  • Angles inside a prism
    r1+r2=Ar_{1} + r_{2} = A
  • Deviation
    δ=i+e−A\delta = i + e - A

Key terms

Angle of deviation

The angle between the direction of the incident ray and the direction of the emergent ray.

Angle of the prism

The angle between the two refracting faces of a prism.

6. Critical angle and total internal reflection

  • Critical angle C: the angle of incidence in the denser medium for which the angle of refraction in the rarer medium is 90∘90^\circ.
  • For a medium in air: μ=1/sin⁡C\mu = 1 / \sin C.
  • Total internal reflection (TIR): when i>Ci > C, all the light is reflected back into the denser medium. Conditions: light travels from denser to rarer; i>Ci > C.
  • Totally reflecting prisms (45°–45°–90° glass, C≈42∘C \approx 42^\circ): enter a short face normally → turned through 90° (periscope); enter the hypotenuse face normally → turned through 180° (binoculars, reflectors). An equilateral prism can also reflect totally at a face.
  • Advantages over a plane mirror: all light reflected (brighter), one image only, no silvering to spoil.
Table of critical angles of water, glass and diamond
MediumC (about)
Water49°
Glass42°
Diamond24°

Formulas

  • Critical angle
    μ=1sin⁡C\mu = \frac{1}{\sin C}

Key terms

Critical angle

The angle of incidence in the denser medium for which the refracted ray grazes the surface (angle of refraction 90°).

Total internal reflection

Reflection of all the light back into a denser medium when it meets the boundary with a rarer medium at more than the critical angle.

Exam tips

Common mistakes

  • Measuring angles from the surface instead of the normal.
  • Saying the frequency of light changes in glass.
  • Writing apparent depth = real depth × μ.
  • Giving only one condition for total internal reflection.
  • Drawing the emergent ray of a glass block not parallel to the incident ray.

How marks are usually awarded

  • Calculations: formula, substitution, answer (and unit where there is one; μ has none).
  • Ray diagrams: arrows on rays, normals drawn dotted, angles labelled, emergent ray direction correct.
  • TIR: both conditions, each with its key word (denser to rarer; greater than the critical angle).