HLT-OPTI68-02 · Lesson 2 · 14 clock hours · demo
Reflection and Refraction at Optical Surfaces
Objective. Students will apply the law of reflection and Snell's Law to predict the behavior of a light ray at a flat optical interface, given the indices of refraction of two media.
⚠ Pending professional review
This lesson, its worked examples and its practice questions has not yet been verified by a licensed clinician in the field or by a certification or approval body. It is a study draft and may contain errors. Do not use it to make decisions about any patient or medication. Always follow your instructor, your supervising professional, and current official references and regulations.
VoTechWorks program approval and accreditation are still in progress. Credentials are issued only by the certifying bodies named in each program, after their own exams.
What Light Does at a Boundary
When a ray of light travels through one material and strikes the surface of a different material, two things can happen simultaneously: some of the light bounces back (reflection) and some of it passes through but changes direction (refraction). Understanding both behaviors is fundamental to every lens you will ever make, measure, or dispense.
The Law of Reflection
Reflection follows a simple, exact rule: the angle of incidence equals the angle of reflection. Both angles are measured from the normal — an imaginary line drawn perpendicular to the surface at the point where the ray strikes. If a ray hits a flat mirror at 30° from the normal, it leaves at 30° on the other side of the normal. This principle applies to any smooth optical surface, including the front curve of a spectacle lens.
For patient safety in the dispensing lane, unwanted reflections off lens surfaces reduce clarity and can cause glare — which is exactly why anti-reflective coatings are prescribed for night driving and for anyone doing extended computer work.
The Index of Refraction
Light travels fastest in a vacuum. In any other medium — air, glass, plastic, water — it slows down. The index of refraction (n) describes how much it slows:
n = speed of light in vacuum ÷ speed of light in the medium
Because light always slows down (or stays the same) when entering a real material, n is always ≥ 1. Key values you will use in opticianry:
- Air: n ≈ 1.000 (treated as 1.000 in calculations)
- Water: n ≈ 1.333
- CR-39 plastic: n = 1.499
- Crown glass: n = 1.523
- Polycarbonate: n = 1.586
- High-index plastics: n = 1.60 and above
Higher-index materials bend light more sharply, which is why high-index lenses can be made thinner for the same prescription.
Snell's Law
The precise relationship between the angle of incidence and the angle of refraction is given by Snell's Law:
n₁ sin θ₁ = n₂ sin θ₂
Where:
- n₁ = index of the medium the ray is coming from
- θ₁ = angle of incidence (measured from the normal)
- n₂ = index of the medium the ray is entering
- θ₂ = angle of refraction (measured from the normal)
What Snell's Law tells you intuitively:
- When light goes from a lower-n to a higher-n medium (e.g., air into glass), it bends toward the normal (θ₂ < θ₁).
- When light goes from a higher-n to a lower-n medium (e.g., glass into air), it bends away from the normal (θ₂ > θ₁).
Always draw the normal first, then measure all angles from it — a common source of error is measuring from the surface itself.
Total Internal Reflection
When light travels from a denser medium (higher n) to a less dense medium (lower n), θ₂ is larger than θ₁. At a specific incident angle — the critical angle — the refracted ray runs exactly along the surface (θ₂ = 90°). Above this critical angle, no light passes through at all: total internal reflection occurs. The critical angle θ_c can be found with:
sin θ_c = n₂ / n₁
Total internal reflection is the physical principle behind fiber-optic instruments used in optometry and ophthalmology, such as slit-lamp illumination systems and certain imaging devices. Light is trapped inside the fiber and guided along its length with virtually no loss. Recognizing how optics principles connect to clinical tools reinforces why this theory matters to your daily work.
Applying This in the Optical Lab
Every time you verify a lens with a lensometer or interpret a prescription, you are relying on the fact that different lens materials refract light predictably and consistently. Choosing the correct lens material for a high-powered prescription involves knowing that polycarbonate (n = 1.586) will produce a thinner lens than CR-39 (n = 1.499) for the same power, because its higher index bends light more efficiently.
Safety Notes
- Ray boxes produce a focused bright beam. Do not direct it toward anyone's eyes. When working with the light table, keep the beam aimed at the optical block only.
- Glass blocks have sharp edges if chipped. Inspect blocks before use; discard any that are cracked or have sharp fragments.
- Calculators and worksheets: double-check that your calculator is in degree mode (not radian mode) before computing any sine or inverse-sine. A radian-mode error produces completely wrong angles and will not be caught by a simple glance at the number.
- Scope of practice reminder: opticians advise patients on lens materials based on their prescription and lifestyle. Material selection that affects safety — such as recommending impact-resistant polycarbonate for children or monocular patients — is a patient-safety decision, not just a cosmetic one.
Key terms8
NormalAn imaginary line drawn perpendicular to an optical surface at the point where a ray strikes it; all angles in reflection and refraction are measured from this line, not from the surface itself.
Angle of Incidence (θ₁)The angle between the incoming light ray and the normal at the point of contact with the surface.
Angle of Refraction (θ₂)The angle between the refracted (transmitted) ray and the normal on the far side of the interface.
Index of Refraction (n)A dimensionless number expressing how much a material slows light compared with a vacuum; equal to the speed of light in a vacuum divided by the speed of light in the medium. Always ≥ 1.
Snell's LawThe mathematical relationship n₁ sin θ₁ = n₂ sin θ₂ that predicts the direction of a refracted ray at the boundary between two media.
Total Internal ReflectionThe complete reflection of a light ray back into a denser medium when it strikes the boundary with a less dense medium at an angle at or beyond the critical angle; no light is transmitted across the boundary.
Critical Angle (θ_c)The minimum angle of incidence (measured from the normal) at which total internal reflection occurs; calculated as sin θ_c = n₂ / n₁ when light travels from n₁ to n₂ where n₁ > n₂.
Law of ReflectionThe physical law stating that the angle of incidence equals the angle of reflection, with both angles measured from the normal to the surface.
Worked examples4
1. A ray of light in air (n = 1.000) strikes the flat surface of a crown glass block (n = 1.523) at an angle of incidence of 35°. What is the angle of refraction inside the glass?
- Write Snell's Law: n₁ sin θ₁ = n₂ sin θ₂
- Substitute known values: (1.000)(sin 35°) = (1.523)(sin θ₂)
- Calculate sin 35° = 0.5736
- Solve for sin θ₂: sin θ₂ = 0.5736 / 1.523 = 0.3766
- Find θ₂: θ₂ = arcsin(0.3766) = 22.1°
Answer: The angle of refraction is approximately 22.1°. The ray bends toward the normal because it entered a denser medium.
2. A ray traveling inside a polycarbonate lens (n = 1.586) hits the back surface where it meets air (n = 1.000) at an angle of incidence of 25°. What is the angle of refraction in air?
- Write Snell's Law: n₁ sin θ₁ = n₂ sin θ₂
- Substitute: (1.586)(sin 25°) = (1.000)(sin θ₂)
- Calculate sin 25° = 0.4226
- Multiply: sin θ₂ = 1.586 × 0.4226 = 0.6702
- Find θ₂: θ₂ = arcsin(0.6702) = 42.1°
Answer: The angle of refraction in air is approximately 42.1°. The ray bends away from the normal because it entered a less dense medium.
3. What is the critical angle for a CR-39 lens (n = 1.499) at its interface with air (n = 1.000)?
- Use the critical angle formula: sin θ_c = n₂ / n₁
- Substitute: sin θ_c = 1.000 / 1.499 = 0.6671
- Find θ_c: θ_c = arcsin(0.6671) = 41.8°
Answer: The critical angle is approximately 41.8°. Any ray inside the CR-39 lens striking the air interface at 41.8° or greater will undergo total internal reflection.
4. A ray in air (n = 1.000) strikes a flat CR-39 surface (n = 1.499) at an angle of incidence of 48°. What angle of refraction results inside the CR-39?
- Write Snell's Law: n₁ sin θ₁ = n₂ sin θ₂
- Substitute: (1.000)(sin 48°) = (1.499)(sin θ₂)
- Calculate sin 48° = 0.7431
- Solve for sin θ₂: sin θ₂ = 0.7431 / 1.499 = 0.4957
- Find θ₂: θ₂ = arcsin(0.4957) = 29.7°
Answer: The angle of refraction inside the CR-39 is approximately 29.7°. The ray bends toward the normal on entering the denser material.
The math in this lesson2
Learners solve n₁ sin θ₁ = n₂ sin θ₂ for the unknown refraction angle.
A-CED.4G-SRT.8
In class: Instructor demonstration using a ray box, glass block, and protractor on a light table: students measure incident and refracted angles at air-glass and air-water interfaces and record data in a structured worksheet. · Paired problem set: 12 Snell's Law calculations using indices for air, crown glass (n = 1.523), CR-39 (n = 1.499), and polycarbonate (n = 1.586); students check answers against an answer key and flag errors for discussion. · Whole-class discussion connecting total internal reflection to fiber-optic instruments used in optometry offices, reinforcing why understanding optics matters clinically.
Materials: Ray box with single-slit aperture, glass and acrylic blocks, protractors, light table, Snell's Law worksheet, scientific calculators, textbook reference chapter on geometric optics
Check: Completed worksheet with all 12 Snell's Law problems attempted; at least 10 correct (83%) to proceed; errors reviewed individually before Lab 1.
Practice check8
Answer each question, then check it. Nothing is recorded; this is your own practice.
Record this lesson on my transcript. Sign in with your key and enrollment email to record lessons (enroll free if you have no key). This page stays open to read and practise.