Reflection Principles Slides Unit: Wave Optics
RE-FLECTION
Mastering the geometry of bouncing light and the predictability of ray diagrams.
Lesson 01 // Geometric Optics
The Challenge: Mirror Maze
Can you make a laser beam hit a target behind a wall using only three mirrors?
Constraints
Fixed source position
Indirect path required
Precision is paramount
The Law of Reflection
The angle of incidence equals the angle of reflection.
\[ \theta_i = \theta_r \]
*Both angles are measured from the Normal (90° from the surface).
NORMAL
\( \theta_i \) \( \theta_r \)
Surface Texture Matters
Specular
Reflection from smooth surfaces where light rays remain parallel.
Example: Mirror, Calm Water
Diffuse
Reflection from rough surfaces where light scatters in many directions.
Example: Paper, Brick Wall
Constructing a Ray Diagram
PHASE 1: DRAWING
1
Draw the surface and the Normal line.
2
Draw the incident ray from the object.
3
Draw the reflected ray using \(\theta_i = \theta_r\).
4
Trace rays behind the mirror (virtual side) with dashed lines.
OBJECT
VIRTUAL IMAGE
Your Turn
Open your Mirror Maze Worksheet. Work with your partner to predict the path of the laser across three reflection points.
Timer 15:00
Mode Collaborative
Mirror Maze Worksheet Mirror Maze Worksheet
Physics 11 // Unit 04: Wave Optics // Lesson 01
Name:
Date:
Part 1: Protractor Proficiency
Measure the angle of incidence (\(\theta_i\)) and predict the angle of reflection (\(\theta_r\)) for the diagrams below. Remember to measure from the Normal (dashed line).
\(\theta_i = \) _________°
\(\theta_r = \) _________° (Predict)
\(\theta_i = \) _________°
\(\theta_r = \) _________° (Predict)
Part 2: The Maze Challenge
Below is a schematic of a laser maze. Your goal is to navigate the beam from the Source to the Target using exactly three mirrors .
Source
Target
Lab Area
Lab Observations
Sketch your mirror placements above. Measure the angles at each contact point below.
Mirror 1 Incidence:
Mirror 2 Incidence:
Mirror 3 Incidence:
Technical Analysis
How did changing the orientation of the first mirror affect the final destination of the beam? Explain using the relationship between incidence and reflection.
Part 3: Ray Diagram Analysis
Construct a full ray diagram for the object below to find the location and orientation of the virtual image . Use a ruler!
OBJECT
REAL SIDE
Virtual Side
Image Distance
Magnification
Orientation Reflection Teacher Guide Teacher Guide
Lesson 01: Reflection & Ray Diagrams
Duration 90 Minutes
Objective
Students will derive \(\theta_i = \theta_r\) and apply geometric principles to predict light paths in a multi-reflection system.
Materials
Laser pointers, flat mirrors (3 per group), protractors, rulers, "Mirror Maze" printouts.
Key Concept
The normal line is the critical reference point for all measurements in geometric optics.
Instructional Sequence
10m
The Hook: Laser Maze
Present the "Mirror Maze" challenge. Darken the room and demonstrate a single reflection. Ask students to predict where the beam will go before turning the laser on.
20m
Direct Instruction
Use the slides to define the Law of Reflection. Stress the importance of the Normal line. Most student errors come from measuring the angle between the mirror and the ray.
45m
Inquiry Lab: Maze Solving
Students work in pairs. They must calculate the required angles for their mirrors on paper before setting up the physical mirrors. This forces the use of the Law of Reflection.
15m
Diagramming & Debrief
Introduce virtual images. Students complete the ray diagram on Part 3 of the worksheet. Discuss: Why are mirrors "reversed"? (Hint: They aren't, they are front-to-back inverted!)
Setup & Safety
Laser Safety: Use Class II lasers. Remind students never to aim at eyes or look directly into the beam source.
Visibility: Use chalk dust or a fog machine (sparingly) to make the laser paths visible in the air.
Stability: Provide small blobs of adhesive putty (Blu-Tack) to hold mirrors upright on the grid paper.
Guiding Questions
"If the angle between the mirror and the beam is 30°, what is the angle of incidence?" (Answer: 60°)
"Why do we draw the normal line at every single point where the beam hits a mirror?"
"If you want to see your feet in a mirror, do you look at the top or the bottom of the mirror? Why?"
Correction Zone: Common Misconceptions
The Angle Reference
Students often measure from the surface of the mirror rather than the normal. Correct this early with the protractor exercise.
Image Location
Students think the image is "on" the mirror's surface. Remind them that the image is behind the mirror, at the same distance as the object is in front.
Refraction and Snell's Law Slides Unit: Wave Optics
RE-FRACTION
Investigating the speed of light through matter and the geometry of bending rays.
Lesson 02 // Snell's Law
The Optical Illusion
Why does a straw look broken when placed in a glass of water?
The Culprit
Light changes speed when it transitions between materials. This causes the path to change direction—a phenomenon called refraction.
AIR (Fast)
WATER (Slow)
Index of Refraction (\(n\))
The index of refraction is a ratio that compares the speed of light in a vacuum (\(c\)) to its speed in a medium (\(v\)).
\[ n = \frac{c}{v} \]
Rule of Thumb:
The higher the \(n\) value, the slower light travels in that material.
Material Index (\(n\)) Vacuum / Air 1.00 Water 1.33 Ethanol 1.36 Crown Glass 1.52 Diamond 2.42
The Equation
SNELL'S LAW
\[ n_1 \sin \theta_1 = n_2 \sin \theta_2 \]
\(n_1\)
Initial Index
\(\theta_1\)
Angle of Incidence
\(n_2\)
Final Index
\(\theta_2\)
Angle of Refraction
Predicting the Bend
Fast to Slow
(Air to Water)
Light bends TOWARD the normal.
\(\theta_2 < \theta_1\)
Slow to Fast
(Glass to Air)
Light bends AWAY from the normal.
\(\theta_2 > \theta_1\)
Refraction Lab
Using semi-circular acrylic blocks and laser boxes, you will measure the entry and exit angles of light to determine the unknown index of refraction for two mystery materials.
Goal Find \(n\)
Precision 0.5 Degrees
Refraction Lab Report Worksheet Refraction Lab Report
Investigation: Snell's Law Verification
Scientist:
Date:
Inquiry Objective
"Determine the relationship between the angle of incidence and the angle of refraction for light passing from air into a denser medium, and calculate the refractive index (\(n\)) using the slope of a linearized data plot."
Constants
- Light Source: Red Diode Laser
- \(n_{air}\) = 1.00
- Temp: 22°C
Table 1: Raw Observation Data
Trial Angle Incidence (\(\theta_1\)) Angle Refract (\(\theta_2\)) \(\sin \theta_1\) \(\sin \theta_2\) 1 10° 0.174 2 20° 0.342 3 30° 0.500 4 45° 0.707 5 60° 0.866
Figure 1: Linearization Analysis
DEPENDENT VARIABLE (\(\sin \theta_2\))
INDEPENDENT VARIABLE (\(\sin \theta_1\))
Slope Calculation
Slope (m) = \(\frac{\Delta \sin \theta_1}{\Delta \sin \theta_2}\)
Based on Snell's Law (\(n_1 \sin \theta_1 = n_2 \sin \theta_2\)), the slope of your line represents the Index of Refraction (\(n_2\)).
Experimental Value (\(n_{exp}\)):
Percent Error (%):
Assume Theoretical \(n = 1.49\)
Critical Synthesis
1. Why is it necessary to measure angles from the Normal line rather than the surface of the acrylic block?
2. If you repeated this experiment with a block of diamond (\(n=2.42\)), how would the slope of your graph change? Explain using your data.
3. Predict: What would happen to the refracted beam if you reached an incident angle of 90°? Is there a limit to how much light can bend? Refraction Teacher Guide Teacher Guide
Lesson 02: Refraction & Snell's Law
Duration 90 Minutes
Lesson Flow
00-15m
The "Broken Straw" Mystery
Demonstration & Hook
15-35m
Refractive Index & Math of Bending
Slides & Worked Examples
35-75m
Snell's Law Verification Lab
Data Collection & Graphing
75-90m
Slope Analysis & Discussion
Synthesis Questions
Lab Facilitation
Acrylic Block Alignment
Students must ensure the laser hits the flat edge of the semi-circular block exactly at the center point. If they hit the curved side first, the light will not refract as expected for a simple Snell's Law calculation.
Graphing Strategy
Encourage students to plot \(\sin \theta_1\) on the Y-axis and \(\sin \theta_2\) on the X-axis. This makes the slope equal to \(n_2\), assuming \(n_1\) (air) is 1.00.
Expected Findings
Index of Acrylic/Lucite
\(n \approx 1.49 - 1.50\)
Linearity
The plot of sines should be perfectly linear. If students get a curve, they are likely measuring angles from the surface, not the normal.
Troubleshooting & Misconceptions
Issue: Light doesn't bend
Check if the laser is entering the block at 0° (along the normal). At \(\theta_i = 0\), \(\theta_r = 0\). Students often think "nothing is happening" and need to be prompted to rotate the light source.
Issue: Calculator Error
Ensure all calculators are in DEGREE mode. Radian mode will produce nonsensical values for sine functions in this lab.
Synthesis Discussion Guide
Q: Does the color of the laser matter?
A: Yes! This is Dispersion . Different wavelengths (colors) of light travel at slightly different speeds in matter. Blue light generally bends more than red light. This is why prisms create rainbows.
Q: What happens if light goes from a slow material to a fast material?
A: Light bends away from the normal. This leads into the next lesson on Total Internal Reflection.
Total Internal Reflection Slides Unit: Wave Optics
TOTAL INTERNAL
REFLECTION
Discovering the boundary where refraction ends and light becomes perfectly trapped.
Lesson 03 // Critical Angles
The Light Fountain
Trapping Light in a Water Stream
Can we make light bend around a corner?
Standard ray optics says light travels in straight lines. However, if we trap light inside a medium using continuous reflection, we can guide it along any path.
Requirement
The light must be moving from a Slow medium to a Fast medium.
The Critical Angle (\(\theta_c\))
As the angle of incidence increases, the refracted ray bends further away from the normal. Eventually, it reaches 90°.
At the Threshold:
\[ \sin \theta_c = \frac{n_2}{n_1} \]
Where \(n_1 > n_2\)
\(n_1\) (Glass)
\(n_2\) (Air)
90°
Total Internal Reflection
When \(\theta_i > \theta_c\), no light escapes. 100% of the energy is reflected back into the first medium.
Better than a mirror: Modern mirrors reflect ~90-95% of light. TIR reflects 100%.
Prismatic binoculars use TIR to fold light paths into small spaces.
NO ESCAPE
ZONE
The Backbone of the Internet
Fiber Optic Cables
Thin strands of glass or plastic that carry digital information using pulses of light.
High Speed (Speed of light in glass!)
No electromagnetic interference
Low signal loss over long distances
Cross-section of an Optical Fiber
The Critical Challenge
Calculate the critical angle for light moving from Diamond (\(n=2.42\)) to Air (\(n=1.00\)). Will it be easier or harder to trap light in diamond compared to glass (\(n=1.50\))?
Time Limit
05:00
Critical Angle Worksheet Critical Angle Challenge
Lesson 03 // Wave Optics // Total Internal Reflection
Student:
Section:
Part 1: The Rulebook
Check the boxes that represent a necessary condition for Total Internal Reflection to occur.
Light travels from a Fast medium to a Slow medium.
Light travels from a Slow medium to a Fast medium.
The angle of incidence (\(\theta_i\)) is LESS than the critical angle (\(\theta_c\)).
The angle of incidence (\(\theta_i\)) is GREATER than the critical angle (\(\theta_c\)).
Part 2: Threshold Calculations
Use the equation \(\theta_c = \arcsin(n_2/n_1)\) to find the critical angle for the following transitions into Air (\(n=1.00\)) .
Material A Water (\(n=1.33\))
→
Show work here...
\(\theta_c = \) _________°
Material B Glass (\(n=1.52\))
→
Show work here...
\(\theta_c = \) _________°
Material C Diamond (\(n=2.42\))
→
Show work here...
\(\theta_c = \) _________°
Part 3: Fiber Optic Logic
Below is a cross-section of a fiber optic cable. A light pulse enters the core (\(n=1.62\)) and strikes the cladding (\(n=1.45\)).
Analysis Questions
1. Calculate the critical angle (\(\theta_c\)) for the Core-Cladding boundary.
2. If the light ray hits the boundary at an angle of 65°, will the signal escape? Why or why not?
Cladding (n=1.45)
Core (n=1.62)
Signal designers want light to stay in the core. If it escapes into the cladding, the data is lost.
Final Synthesis
Diamonds have a very low critical angle (~24°). Explain how this physical property, combined with the way a diamond is faceted (cut), contributes to the "sparkle" or "fire" of the gemstone.
TIR Teacher Guide Teacher Guide
Lesson 03: Total Internal Reflection
Duration 60-90 Minutes
Lesson Strategy
This lesson marks the transition from simple refraction to the phenomenon of light trapping. It is highly visual and relies on the "Light Fountain" demonstration to solidify student intuition before moving into the math of critical angles.
Key Demos
The Light Fountain: Poke a hole in a clear plastic bottle filled with water. Aim a laser through the back of the bottle into the stream of water. The light will follow the curve of the water.
The Invisible Coin: Place a coin in a glass of water. Look from the side at a sharp angle—the coin disappears because light is reflected off the top surface of the water back down.
Mathematical Focus
Derive the critical angle formula by setting \(\theta_2 = 90^\circ\) in Snell's Law:
\(n_1 \sin \theta_c = n_2 \sin 90^\circ\)
\(n_1 \sin \theta_c = n_2 (1)\)
\(\sin \theta_c = \frac{n_2}{n_1}\)
Reminder: This only works if \(n_1 > n_2\). Otherwise, \(\sin \theta_c > 1\), which is undefined.
Discussion Prompts
Why is fiber optics preferred over copper wire?
Light can carry significantly more data than electricity (higher bandwidth) and isn't affected by magnetic fields. Since TIR is 100% efficient, signal loss is minimal compared to resistance in wires.
How do mirages on hot roads work?
Hot air near the road is less dense than the cooler air above it. As light from the sky moves toward the road, it moves from dense to less dense air (Slow to Fast). If the angle is shallow enough, TIR occurs, reflecting the sky and looking like water on the road.
Answer Key Summary
Part 2: Calculations
Water (\(n=1.33\)): \(\theta_c \approx 48.8^\circ\)
Glass (\(n=1.52\)): \(\theta_c \approx 41.1^\circ\)
Diamond (\(n=2.42\)): \(\theta_c \approx 24.4^\circ\)
Part 3: Fiber Optics
\(\theta_c\) for Core-Cladding: \(\theta_c = \arcsin(1.45/1.62) \approx 63.5^\circ\)
Scenario: 65° is greater than the critical angle (63.5°), so TIR will occur and the signal is safely trapped.
Part 4: Diamond Sparkle
Because diamond has such a low critical angle, light that enters is much more likely to be totally internally reflected rather than passing out the bottom. The "fire" is caused by multiple reflections inside the stone before the light eventually exits through the top facets, splitting into colors (dispersion) along the way.
Diffraction and Interference Slides Unit: Wave Optics
DIFFRACTION & INTERFERENCE
Proving the wave nature of light through bending around obstacles and the collision of wavefronts.
Lesson 04 // Physical Optics
The Ray Paradox
Ray optics tells us that light travels in straight lines.
If you shine a laser through a microscopic slit, you should see a single tiny dot of light.
What actually happens?
The light spreads out into a wide pattern of bands. It behaves like water waves passing through a harbor opening.
Single Slit Observation
Huygens' Principle
Every point on a wavefront acts as a source of tiny spherical wavelets.
The new wavefront is the surface that is tangent to all of these wavelets. This explains why light "bends" into the shadow region of an obstacle.
Key Definition
Diffraction:
The bending of waves around the edge of an obstacle or through an aperture.
Collision of Waves
CONSTRUCTIVE
(Crest Meets Crest)
Waves add together to create a BRIGHT BAND.
DESTRUCTIVE
(Crest Meets Trough)
Waves cancel out to create a DARK BAND.
The Double Slit Experiment
Thomas Young (1801) used two slits to create two coherent sources of light wavelets.
The Evidence
The resulting pattern of bright and dark fringes on a screen proved that light is WITHOUT A DOUBT a wave.
Interference Fringe Pattern
Fringe Finder
Open your Interference Analysis Worksheet. We will use laser-diffraction slides to measure the distance between interference bands and calculate the wavelength (\(\lambda\)) of light.
Equation \(d \sin \theta = m \lambda\)
Target Variable Wave-length
Interference Analysis Worksheet Interference Pattern Analysis
Lab Log // Wavefront Interactions
Station:
Lead:
Part 1: Superposition Warm-up
Sketch the Resultant Wave when the two input waves collide at the center point. Indicate if the interference is Constructive or Destructive .
Scenario A: In-Phase
Resultant Wave
Type: ______________
Scenario B: 180° Out-of-Phase
Resultant Wave
Type: ______________
Part 2: Fringe Geometry
Using the laser-diffraction slide, observe the pattern projected on the screen. Measure the following values to calculate the wavelength (\(\lambda\)).
Slit Separation (\(d\)) 0.125 mm
Distance to Screen (\(L\))
Fringe Spacing (\(\Delta y\))
The Small Angle Approximation
\[ \lambda = \frac{d \cdot \Delta y}{L} \]
*Ensure all units are converted to Meters before calculating.
Lab Schematic
Distance L
Fringe Space \(\Delta y\)
Calculation for \(\lambda\):
Predictive Modeling
Variable Change
You swap the red laser (\(\lambda=650nm\)) for a green laser (\(\lambda=532nm\)).
Will the fringes get closer or further apart?
Variable Change
You move the screen significantly further away from the slits (increase \(L\)).
Will the fringes get wider or narrower?
Variable Change
You use a slide with more closely spaced slits (decrease \(d\)).
How does this affect the pattern spacing?
Diffraction Teacher Guide Teacher Guide
Lesson 04: Diffraction & Interference
Topic Physical Optics
Instructional Roadmap
Phase 1
Superposition Hook
Demo wave addition on a Slinky or water tank. (10m)
Phase 2
Double Slit Proof
Historical context of Young's Experiment. Theory of path difference. (20m)
Phase 3
Fringe Lab
Measuring \(\Delta y\) and \(L\) to calculate \(\lambda\). (45m)
Phase 4
Synthesis
Connecting pattern width to wavelength/slit size. (15m)
Lab Setup & Tips
Averaging Fringes
To increase precision, have students measure the distance across 10 bright fringes and then divide by 10 to find \(\Delta y\). Measuring a single fringe is prone to high error.
Room Conditions
Complete darkness is required. If your room has windows, use black-out curtains or perform the lab in a large hallway/closet area.
The Small Angle Assumption
Remind students that \(y/L\) is only a valid substitute for \(\sin \theta\) when the distance to the screen is significantly larger than the fringe spacing.
Wavelength Targets
Expected values for standard educational lasers:
Red Diode
Standard
630 - 670 nm
Green Diode
High Precision
532 nm
Violet Diode
Rare/Optional
405 nm
Simulation Guide (PhET)
If physical lasers are unavailable, use the PhET 'Wave Interference' simulation (Slits screen).
Investigation 1
Wavelength Shift
Have students slide the color bar from Red to Blue. Observe how the pattern 'crunches' together for shorter wavelengths.
Investigation 2
Slit Separation
Change the distance between slits. Students should note that as slits move closer , the interference pattern gets wider .
Correction Zone: Common Misconceptions
Unit Conversion Nightmare
Students will forget to convert mm and cm to meters. This will lead to wavelengths that are off by several powers of ten. Provide a conversion table on the board.
Diffraction vs Interference
Clarify that diffraction is the bending of the wave as it passes the slit, while is what happens when those bent waves overlap. The double slit pattern is actually an interference pattern enveloped by a diffraction pattern.
Polarization Slides Unit: Wave Optics
POLARIZATION
Controlling the direction of oscillation to manage glare, display images, and analyze structural stress.
Lesson 05 // Transverse Waves
The Magic Filter
BLACKOUT
Crossed Polarizers
Why do two clear filters make complete darkness?
Light is a transverse wave, meaning it vibrates in many directions at once. Polarization is the process of restricting light to vibrate in a single plane.
Observation
Rotate your 3D glasses in front of a computer screen. What happens at 90 degrees?
Transverse Waves only
Only Transverse waves (like EM waves) can be polarized.
Longitudinal waves (like Sound) vibrate along the same direction they travel, so they cannot be filtered by orientation.
The Slat Analogy
Think of a rope being shaken through a picket fence. If the shake is vertical and the slats are vertical, the wave passes. If the shake is horizontal, it is blocked.
Unpolarized (Random) vs Polarized (Aligned)
Technology & Polarization
LCD Screens
Use liquid crystals to rotate polarized light to turn pixels "on" or "off".
Sunglasses
Glare from water or roads is horizontally polarized. Vertical filters block it 100%.
Stress Analysis
Engineers use polarized light to see internal stress patterns in plastic prototypes.
Brewster's Angle
When unpolarized light hits a non-metallic surface at a specific angle, the reflected light becomes perfectly polarized.
\[ \tan \theta_p = \frac{n_2}{n_1} \]
This is why polarized sunglasses are so effective at removing the "shine" from the surface of a lake.
POLARIZED GLARE
Tech Case Study
Open your Polarization & Technology Worksheet. You will investigate how LCD pixels rotate light and analyze the "Brewster's Angle" of a mystery surface.
Mode Investigation
Skills Evidence Analysis
Polarization Worksheet Polarization & Tech
Case Study // Transverse Wave Applications
Analyst:
Date:
Part 1: The Transverse Requirement
Explain why sound waves (longitudinal) cannot be polarized while light waves (transverse) can. Use the "Slat and Rope" analogy discussed in the lesson.
Write your explanation here...
Part 2: Engineering an LCD Pixel
Vertical Polarizer
Liquid Crystal
Horizontal Polarizer
Analysis Task
In a laptop screen, these two filters are permanently "crossed" (one vertical, one horizontal). Why is it that you can still see an image? What must the liquid crystal be doing to the light as it passes through the middle layer?
Part 3: Brewster's Angle Optimization
A photographer wants to remove the reflection of the sky from the surface of a swimming pool (\(n=1.33\)).
1. Calculate the Brewster's Angle (\(\theta_p\)) for the air-water interface.
Show work using \(\tan \theta_p = n_2 / n_1\)
2. If the reflected glare is horizontally polarized, in which orientation should the photographer rotate their polarizing camera filter to block it?
Vertical
Horizontal
Technical Insight
When light is reflected at Brewster's Angle, the reflected and refracted rays are exactly 90 degrees apart. This prevents the oscillation from continuing into the reflection in any direction other than parallel to the surface.
Quality Control Analysis
Engineers use a technique called Photoelasticity . When clear plastic is under stress, it becomes "birefringent," meaning it rotates polarized light differently at different stress points. When viewed through a second polarizer, colorful bands appear.
Predict: Where would the colors be most dense and vibrant on a plastic bridge prototype? (At the supports or in the middle of a span? Why?)
Polarization Teacher Guide Teacher Guide
Lesson 05: Polarization Experimentation
Unit Final EM Waves
Unit Culmination
This lesson connects wave theory to ubiquitous technology. It provides a definitive proof of the transverse nature of light and explains how we manipulate wave orientation for functional purposes.
Experimental Stations
Station 1: Screen Blackout. Rotate a single polarizing filter in front of an LCD laptop screen. At ~90°, the screen will go black.
Station 2: Glare Removal. Place a polarizing filter over a reflective surface (like a glass table). Rotate to find the angle where the reflection disappears.
Station 3: 3D Vision. Provide RealD 3D glasses. Note that they use circular polarization, but for 11th grade, treat them as linear (one vertical, one horizontal) for simplicity.
The Brewster Detail
Brewster's Angle occurs when the reflected ray and refracted ray are perpendicular.
\(n_1 \sin \theta_p = n_2 \sin \theta_r\)
If \(\theta_p + \theta_r = 90^\circ\), then:
\(n_1 \sin \theta_p = n_2 \cos \theta_p\)
\(\tan \theta_p = \frac{n_2}{n_1}\)
Instructional Nuance
How LCDs Work (The "Twisted Nematic" Effect)
Many students struggle with why light passes through crossed polarizers. Explain that the liquid crystal molecules are physically twisted. When the power is off , they "untwist" the light by 90°, allowing it to pass through the second filter. When the power is on , they align, no rotation occurs, and the light is blocked (black pixel).
Polarization by Scattering
Explain why the sky is blue and partially polarized. Sunlight hitting air molecules scatters more blue light. Because the scattering occurs at 90 degrees relative to the sun, the light reaching your eyes from certain parts of the sky is polarized. This is why photographers use "Polarizers" to make the sky look deeper blue.
Analysis Key Summary
Part 2: LCD Logic
The liquid crystal must be rotating the plane of polarization by 90 degrees. Without this rotation, the second (horizontal) polarizer would block all the light coming from the first (vertical) polarizer.
Part 3: Glare & Brewster
Brewster Calculation: \(\theta_p = \arctan(1.33/1.00) \approx 53.1^\circ\)
Filter Orientation: Vertical . Horizontal glare (glare from a horizontal surface) can only be blocked by a vertical picket-fence style filter.