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The Calculus of Rainbows By Angela Han, Rabeea Abbas, Laura Boardman, and Cathy Ma

The Calculus Of Rainbows[1]Completepresentyay

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Page 1: The Calculus Of Rainbows[1]Completepresentyay

The Calculus of

RainbowsBy Angela Han, Rabeea Abbas, Laura

Boardman, and Cathy Ma

Page 2: The Calculus Of Rainbows[1]Completepresentyay

Rainbow History• Early attempts to explain the rainbow

through myths:– Ancint Greece- the goddess Iris used

the rainbow as a sign of both warning and hope

– Africa- rainbow was a large snake coming out to graze after the storm, again a symbol of both hope and fear

– Australian aboriginals- Rainbow serpent Is the Creator that can give fertility by creating rain but also let loose blindness and disease

– Native Americans- a bridge anchored in this world and leading to the next

• Today we can determine the cause of rainbows using calculus applied to the properties of light

Page 3: The Calculus Of Rainbows[1]Completepresentyay

The Basics

Fermat’s Principle:

The light which reaches your eye is the light which has traveled

along the quickest path from it’s source

Law of Refraction

Law of Reflection

• Reflection and

reflection are two

manifestations of

Fermat’s Principle

•Fermat’s Principle:

The light which reaches

your eye is the light

which has traveled

along the quickest path

from it’s source

Page 4: The Calculus Of Rainbows[1]Completepresentyay

Reflection Using Fermat’s principle (light follows path that minimizes the

total travel time) we can derive the angle at which light will be reflected

Suppose a source of light rays at point P and passes through pointQ after reflection off the mirror. At what point R does the ray reflect off the mirror?

Using Fermat's principle we know the ray follows a path that minimizes the time necessary to travel from P to Q. Since the speed of light is constant, we can use the triangle in the figure to get the following expression for the path as a function of x: L(x) = √(p²+x²) + √(q²(d-x²)).

To find the minimum path length we find the derivative L’(x): j

Then we set this expression equal to 0: x/(√(p² + x²)) = (d – x)/(√q² + (d – x)²)

Referring to the figure, we see that:

Therefore L’(x) = 0 when cos = cos this is the minimum path length

So…. The Law of Reflection: For reflection, the angle of incidence ( ) equals the angle of

reflection ( )

d

x (d-x)R

Q

P

pq

Page 5: The Calculus Of Rainbows[1]Completepresentyay

Refraction• With reflection, we assumed that

the light rays maintained a constant speed, as the rays traveled through a fixed medium

• What happens if part of the light’s path is in water and part is in air?

P = source of light rays in the airQ = point in waterR = point at which a light ray crosses

the air/water interfaceα = angle of incidenceβ = angle of refraction• The Law of Refraction states that

the ratio of the angle of incidence to the sine of the angle of refraction is a constant

(sinα)/(sinβ)=k

Page 6: The Calculus Of Rainbows[1]Completepresentyay

The Law of Refraction• The total time the light takes to travel

from R to Q is displayed as, where ca

is the speed in air, and cw is the speed in water:

• To find the minimum of, we need to first derive T(x)

• Then we set T’(x) to the 0, which gives:

• This is a constant ratio, known as the index of refraction. For water this value is approximately 1.33.

Page 7: The Calculus Of Rainbows[1]Completepresentyay

The Rainbow Angle• Rainbows form when light strikes a raindrop

and some of it is reflected at the interface or refracted.

• The Law of Refraction states that the light ray that strikes the drop will be bent toward the perpendicular line.

• Generally, as light travels form one medium to another, art of the light is reflected, as the other part continues to another medium, where it’s refracted.

• It is reasonable to think of a water drop as a spherical shape:

• The radius through A is the perpendicular and α is the angle of incidence and β is the angle of refraction.

Page 8: The Calculus Of Rainbows[1]Completepresentyay

The Rainbow Angle cont.

• Point A, the source of light, can be positioned anywhere on the left half of the

circle.

– For example, if A is on the upper half of the raindrop, the ray will exit on the lower half

• If the ray enters the drop along the circle’s diameter, the angle of incidence

and refraction will both be zero; the total deflection will be 180 degrees

• However, as the ray from Point A in figure 2 cross the drop, the deflection

angle changes

• The angle of deflection is a function of the angle of incidence, given by

D(α) = α- β+180-2β+α-β=180+2α-4β

• D(α) is expressed in terms of two variables, α and β, but from the Law of

Refraction (sinα)/(sinβ)=k, β can be expressed as a function

of α

Page 9: The Calculus Of Rainbows[1]Completepresentyay

Rainbow angle continued

• Surprisingly, D(α) only decreases a certain amount, then

suddenly increases.

• Find D’(α), set it to 0, recall that

• Therefore

• Solving this equation in terms of cosα yields:

Page 10: The Calculus Of Rainbows[1]Completepresentyay

Solving a problem involving Calculus• This problem is trying to derive Snell’s

Law of Refraction using Lagrange Multipliers, which are useful for calculating minima or maxima for functions with subject to constraints(a condition that a solution to an optimization problem must satisfy.)

• Lagrange multipliers are denoted by a new variable (λ), and the function is denoted by

Page 11: The Calculus Of Rainbows[1]Completepresentyay