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Lesson 1: Refraction at a Boundary

Boundary Behavior

Refraction and Sight

The Cause of Refraction

Optical Density and Light Speed

The Direction of Bending

If I Were an Archer Fish


Lesson 2: The Mathematics of Refraction

The Angle of Refraction

Snell's Law

Ray Tracing and Problem-Solving

Determination of n Values


Lesson 3: Total Internal Reflection

Boundary Behavior Revisited

Total Internal Reflection

The Critical Angle


Lesson 4: Interesting Refraction Phenomena

Dispersion of Light by Prisms

Rainbow Formation

Mirages


Lesson 5: Image Formation by Lenses

The Anatomy of a Lens

Refraction by Lenses

Image Formation Revisited

Converging Lenses:

Ray Diagrams

Object-Image Relations

Diverging Lenses:

Ray Diagrams

Object-Image Relations

The Mathematics of Lenses


Lesson 6: The Eye

The Anatomy of the Eye

Image Formation and Detection

The Wonder of Accommodation

Farsightedness and its Correction

Nearsightedness and its Correction


Lesson 1: Refraction at a Boundary

The Cause of Refraction

We have learned that refraction occurs as light passes across the boundary between two medium. Refraction is merely one of several possible boundary behaviors by which a light wave could behave when it encounters a new medium or an obstacle in its path. The transmission of light across a boundary between two media is accompanied by a change in both the speed and wavelength of the wave. The light wave not only changes directions at the boundary, it also speeds up or slows down and transforms into a wave with a larger or a shorter wavelength. The only time that a wave can be transmitted across a boundary, change its speed, and still not refract is when the light wave approaches the boundary in a direction which is perpendicular to it. As long as the light wave changes speed and approaches the boundary at an angle, refraction is observed.

But why does light refract? What is the cause of such behavior? And why is there this one exception to the refraction of light? An analogy of marching soldiers is often used to address this question. In fact, it is not uncommon that the analogy be illustrated in a Physics class with a student demonstration. A group of students forms a straight line (shoulder to shoulder) and connect themselves to their nearest neighbor using meter sticks. A strip of masking tape divides the room into two media. In one of the media (on one side of the tape), students walk at a normal pace. In the other media (or on the other side of the tape), students walk very slowly using baby steps. The group of students walk forward together in a straight line towards the diagonal strip of masking tape. The students maintain the line as they approach the masking tape. When an individual student reaches the tape, that student abruptly changes the pace of her/his walk. The group of students continue walking until all students in the line have entered into the second medium. The diagram below represents the line of students approaching the boundary (the masking tape) between the two medium. On the diagram, an arrow is used to show the general direction of travel for the group of students in both medium. Observe that the direction of the students changes at the "boundary."

The fundamental feature of the students' motion which leads to this change in direction is the change in speed. Upon reaching the masking tape, each individual student abruptly changes speed. Because the students approach the masking tape at an angle, each individual student reaches the tape at a different time. The student who reaches the tape first, slows down while the rest of the line of students marches ahead. This occurs for every student in the line of students. Once a student reaches the boundary, that student slows down while his/her nearest neighbor marches ahead at the original pace. The result is that the direction that the line of students is heading is altered at the boundary. The change in speed of the line of students causes a change in direction.

 

Conditions of Refraction

Will this refractive behavior always occur? No! There are two conditions which are required in order to observe the change in direction of the path of the students:

  • The students must change speed when crossing the boundary.
  • The students must approach the boundary at an angle; refraction will not occur when they approach the boundary head-on (i.e., heading perpendicular to it).

These are both reasonable enough conditions if you consider the previous paragraph. If the students do not change speed, then there is no cause factor. Recall that it was the change in speed of the students which caused the change in direction. The second condition is also reasonable. If the students approach the masking tape in a direction which is perpendicular to it , then each student will reach the tape at the exact same time. Recall that the line of student changed their direction because they had reached the masking tape at different times. The first student reached the tape, slowed down, and observed the rest of the students marching ahead at the original speed. The change in direction of the line of students only occurs at the boundary when the students change speed and approach at an angle.

 

The Marching Soldiers analogy provides an excellent analogy to understanding the cause of light refraction. The line of students approaching the masking tape are analogous to a wavefront of light. The masking tape is analogous to a boundary between two medium. The change in speed which occurred for the line of students would also occur for a wave of light. And like the marching students, a light wave will not undergo refraction if it approaches the boundary in a direction which is perpendicular to it.

The same two conditions which are necessary for bending the path of the line of students are also necessary for bending the direction of a light ray. Light refracts at a boundary because of a change in speed. Their is a distinct cause-effect relationship. The change in speed is the cause and the change in direction (refraction) is the effect.

 

 

 

 

Lesson 1: Refraction at a Boundary

 

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