CortexHSC

Year 11 Physics · Waves · Wave behaviours · 13 min read

Refraction and Snell's law

Light bends when it crosses from one material into another: a straw looks broken in a glass of water, and a pool looks shallower than it is. This is refraction, and it happens because light travels at different speeds in different materials.

This guide covers what Year 11 Physics asks you to do with light at a boundary: the law of reflection, the refractive index n = c/v, Snell's law, the critical angle and total internal reflection (the physics of optical fibres). Then come the common mistakes, a quick quiz and a full worked example. One rule runs through all of it: every angle is measured from the normal.

What you need to know

The equations you will use:

nx = c ÷ vxRefractive index of medium x. c = 3.00 × 108 m s−1. n has no unit and is never less than 1.
n1 sin θ1 = n2 sin θ2Snell's law. Medium 1 is where the light comes from. Both angles are measured from the normal.
sin θc = n2 ÷ n1Critical angle, for light going from the higher index n1 to the lower index n2.
angle of incidence = angle of reflection not on the data sheetThe law of reflection, both angles from the normal. It is a rule in words, not a data-sheet equation.

Dot points: PY11-WV-19, PY11-WV-20, PY11-WV-21, PY11-WV-22, PY11-WV-23, PY11-WV-24, PY11-WV-25, PY11-WV-26, PY11-WV-27, PY11-WV-28 (2025 Physics syllabus, Year 11), in our own words.

Mini lesson

Reflection: the normal comes first

The normal is a line drawn at 90° to a surface, at the point where the ray hits it. The law of reflection says the angle of incidence equals the angle of reflection, with both measured from the normal, and the incident ray, reflected ray and normal all lie in the same plane.

You see it in a bathroom mirror, in a still lake, in a periscope (two mirrors at 45°) and in a bike reflector. A smooth surface reflects a parallel beam as a parallel beam, so you see an image. A rough surface (paper, a wall) still obeys the law at every tiny patch, but the normals point every which way, so the light scatters and you see no image.

A ray hits a plane mirror and reflects. A dashed normal stands at right angles to the mirror where the ray hits, and the angle of incidence i and the angle of reflection r are marked on either side of it.irnormalincident rayreflected rayplane mirror
Law of reflection: i = r, both measured from the normal (the dashed line), never from the mirror.

Why light bends: it changes speed

Light travels at c = 3.00 × 108 m s−1 in a vacuum (air is so close that we use n = 1.00) and more slowly in water, glass and plastic. The refractive index says how much slower: n = c ÷ v. Glass with n = 1.50 slows light to 3.00 × 108 ÷ 1.50 = 2.00 × 108 m s−1. A higher n means slower light.

A wavefront diagram shows why the change of speed bends the ray. One side of each wavefront reaches the boundary first and slows down while the rest is still moving fast, so the wavefront pivots. The frequency stays the same (it is set by the source), so the slower wave has a shorter wavelength (v = fλ), and the wavefronts bunch up.

Straight wavefronts approach a flat air-glass boundary at an angle. In the glass the wavefronts are closer together and turned, and the ray drawn at right angles to them bends towards the dashed normal.air: fasterglass: slower
Wavefronts (grey) and a ray (orange). In the glass the wave is slower, so the wavelength is shorter and the ray turns towards the normal. The ray is always at 90° to the wavefronts.

Snell's law

Snell's law turns that bending into numbers: n1 sin θ1 = n2 sin θ2. Medium 1 is the one the light is leaving and θ1 is the angle of incidence; θ2 is the angle of refraction. Both are measured from the normal.

For example, light in air hits glass (n = 1.50) at 50° to the normal: sin θ2 = 1.00 × sin 50° ÷ 1.50 = 0.511, so θ2 = 30.7°. It went into a higher n, so it bent towards the normal: the angle got smaller, as it should.

A ray in air meets a glass surface at angle theta 1 from the dashed normal and continues into the glass at a smaller angle theta 2 from the normal. The air is labelled n 1 = 1.00 and the glass n 2 = 1.50.θ1θ2n1 = 1.00 (air)n2 = 1.50 (glass)
θ1 = 50° in air becomes θ2 = 30.7° in glass. Both angles sit between the ray and the normal.

Critical angle and total internal reflection

When light goes from a higher n into a lower n (glass into air), it bends away from the normal. Make the angle of incidence bigger and the refracted ray swings out until it runs along the surface at 90°. That angle of incidence is the critical angle θc: put θ2 = 90° into Snell's law and you get sin θc = n2 ÷ n1. For glass (1.50) into air, sin θc = 1.00 ÷ 1.50, so θc = 41.8°.

Above the critical angle no light gets out: all of it reflects back inside. This is total internal reflection (TIR), and it needs two conditions: the light must be going towards a lower n, and the angle of incidence must be greater than θc. An optical fibre uses it: a glass core with a lower-n cladding around it, so light meeting the wall above θc reflects again and again along the fibre with almost no loss. That is how internet signals and medical endoscopes carry light around bends.

Three panels of a ray inside glass meeting the glass-air surface. Below the critical angle it refracts out into the air with a faint reflection; at the critical angle it runs along the surface; above the critical angle it reflects totally back into the glass.airglassθ < θcθ = θcθ > θc
Light inside glass hitting the surface at 30°, 41.8° (the critical angle) and 60°. Above θc nothing escapes: total internal reflection.

Measuring a refractive index

The standard experiment shines a ray box beam into a semicircular or rectangular glass (or perspex) block. Trace the block, mark the rays, draw the normal, and measure the angle in air (θair) and in the block (θblock) for five or more angles of incidence.

Plot sin θair on the y-axis against sin θblock on the x-axis. Snell's law with nair = 1.00 says sin θair = n sin θblock, so the points lie on a straight line through the origin and the gradient is n. A ruled line of best fit uses all the data, which beats working out n from one pair of angles.

To assess accuracy, compare your n with the accepted value (perspex is about 1.49) as a percentage difference. Thick pencil lines, a wide beam and a protractor read to ±1° are the usual sources of error, and they matter most at small angles.

Common mistakes

Mini quiz

5 quick questions. Pick an answer to see if you're right and why.

  1. The refractive index of a type of glass is 1.50. What is the speed of light in it?
    Show answer

    C. v = c ÷ n = 3.00 × 108 ÷ 1.50 = 2.00 × 108 m s−1. Multiplying by n gives 4.50 × 108, faster than light, which can't be right.

  2. A ray in air strikes a flat glass surface (n = 1.50) at 60° to the surface. What is the angle of refraction, measured from the normal?
    Show answer

    A. From the normal the angle of incidence is 90° − 60° = 30°. sin θ2 = sin 30° ÷ 1.50 = 0.333, so θ2 = 19.5°. Using 60° directly gives 35.3°, the classic trap.

  3. Which situation can produce total internal reflection?
    Show answer

    B. TIR needs light heading towards a lower refractive index (glass to air) and an angle of incidence greater than θc. Air into glass always refracts in, bending towards the normal.

  4. Diamond has a refractive index of 2.42. What is the critical angle for light inside diamond meeting air?
    Show answer

    A. sin θc = 1.00 ÷ 2.42 = 0.413, so θc = 24.4°. 65.6° is the angle from the surface, and 41.8° is the value for ordinary glass (n = 1.50). The small critical angle is why diamonds sparkle: most light inside reflects.

  5. Light passes from air into water. Which property of the light stays the same?
    Show answer

    C. The source sets the frequency, and a boundary can't change it. The speed drops, so the wavelength gets shorter (v = fλ), and the direction changes unless the ray is along the normal.

Worked example

A diver underwater points a torch up at the flat surface of a swimming pool. The beam meets the surface at an angle of incidence of 28°. The refractive index of water is 1.33 and of air is 1.00.

(a) Calculate the angle the beam makes with the normal after it leaves the water. (3 marks)

(b) Calculate the largest angle of incidence at which the beam can still leave the water. (2 marks)

(5 marks)

I'll think out loud, the way you should in the exam, using KNOW-UD: Knowns, Not known, Organise, Work it out, Units, Direction.

Prediction first. The beam goes from water into air, a lower n, so it bends away from the normal: the angle in air will be bigger than 28°. sin 28° is about 0.47, and multiplying by 1.33 gives about 0.62, so I expect just under 40°. For (b), sin θc = 1.00 ÷ 1.33 is 0.75, so the critical angle should be between 45° and 50°.

K · Knowns

I draw the surface and the normal first, then put the angle on the water side, because that's where the beam starts. The water is medium 1 because the light is leaving it.

  • n1 = 1.33 (water), n2 = 1.00 (air)
  • θ1 = 28° (from the normal)
Sketch of the torch beam: it travels up through water at 28 degrees to a dashed vertical normal, reaches the flat surface and continues into the air at an unknown angle theta 2 from the normal. Water is labelled n = 1.33 and air n = 1.00.28°θ2 = ?airn = 1.00watern = 1.33normal
Knowns on the sketch: water n1 = 1.33, air n2 = 1.00, angle of incidence 28° from the normal. Unknowns: θ2 and the critical angle θc.

N · Not known

Part (a) wants an angle in the air, and part (b) wants the critical angle for water to air. Both answers are angles from the normal, in degrees.

  • (a) θ2 = ?
  • (b) θc = ?

O · Organise

Snell's law links the two angles, so I rearrange it for sin θ2 before I put any numbers in. For (b), the beam can still just leave when the refracted ray runs along the surface, which is the critical angle. Water to air is towards a lower n, so a critical angle exists.

  • (a) n1 sin θ1 = n2 sin θ2 → sin θ2 = n1 sin θ1 ÷ n2
  • (b) sin θc = n2 ÷ n1

W · Work it out

Calculator in degrees first. I keep the full sine values and only round the angles at the end.

  • (a) sin θ2 = 1.33 × sin 28° ÷ 1.00 = 1.33 × 0.46947 = 0.62440
  • θ2 = sin−1(0.62440) = 38.64°
  • (b) sin θc = 1.00 ÷ 1.33 = 0.75188
  • θc = sin−1(0.75188) = 48.75°

U · Units

Both are angles, so degrees. The data are to two or three significant figures, so I give the angles to the nearest tenth of a degree, which is the precision a protractor-based answer can carry.

  • (a) θ2 ≈ 38.6°
  • (b) θc ≈ 48.8°

D · Direction

An angle needs its reference line, so I say 'from the normal'. As a sense check on (a): the light sped up going into air, so it should bend away from the normal, and 38.6° is bigger than 28°. Good. For (b), any angle of incidence bigger than 48.8° gives total internal reflection, so the diver would see the beam reflect back down.

  • (a) 38.6° from the normal, bent away from it
  • (b) 48.8° from the normal; above this the beam is totally internally reflected

(a) The beam leaves the water at 38.6° to the normal. (b) The largest angle of incidence that still lets the beam out is the critical angle, 48.8°.

Check against the prediction. I predicted just under 40° for (a) and between 45° and 50° for (b). 38.6° and 48.8° fit both, and the angle in air is bigger than the angle in water, as it must be for light speeding up.

Exam advice

What markers look for

Summaries in our own words. Read NESA's own feedback with the exam packs: 2025.

Where this leads in Year 12

Light comes back in Year 12 when you test models of light: double-slit interference, diffraction and polarisation support the wave model, you measure the speed of light, and photons link frequency to energy with E = hf. The idea from this topic that carries straight through is that light's speed in a medium sets how it behaves at a boundary, and that frequency is fixed by the source while wavelength changes.

FAQ

Is Snell's law on the data sheet?
Yes. NESA's sample data sheet for the new (2025) syllabus includes nx = c ÷ vx, n1 sin θ1 = n2 sin θ2 and sin θc = n2 ÷ n1. The law of reflection is not an equation, so learn it in words. Check which sheet your school gives you for Year 11 exams.
What is the difference between reflection and refraction?
Reflection is light bouncing off a surface and staying in the same medium, with the angle of incidence equal to the angle of reflection. Refraction is light passing into a new medium and changing direction because its speed changes.
Why do you measure angles from the normal and not the surface?
Because the laws are written that way: Snell's law and the law of reflection only work with angles from the normal. The normal also works for curved surfaces, where 'the surface' has no single direction.
Does light bend towards or away from the normal?
Towards the normal when it goes into a higher refractive index and slows down (air into glass). Away from the normal when it goes into a lower refractive index and speeds up (water into air).
What are the two conditions for total internal reflection?
The light must be travelling towards a medium with a lower refractive index, and its angle of incidence must be greater than the critical angle.

Related guides

Explore more of CortexHSC

CortexHSC is a free Year 11 Physics study app built by a NSW Physics teacher. Pick up where this guide leaves off:

Free to start, no card needed. Some features need a free account; a few are part of a paid pass.