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The figure shows a slender arrow pointing out of the page and to the right; it is labeled direction of ray (of propagation). At a point on this ray, eight bold arrows point in different directions, perpendicularly away from the ray. These arrows are labeled E.
The slender arrow represents a ray of unpolarized light. The bold arrows represent the direction of polarization of the individual waves composing the ray. Since the light is unpolarized, the arrows point in all directions.
The figure shows a slender arrow pointing out of the page and to the right that is labeled direction of ray. At the left end of the ray are eight blue arrows emanating from a point on the ray. These arrows are all in a plane perpendicular to the ray and are symmetrically oriented in the perpendicular plane. They are labeled E. Farther to the right on the same ray is a thin rectangle labeled polarizing filter that is in the plane perpendicular to the ray. This filter has seven vertical lines that are equally spaced on its surface. It also has a vertical double headed arrow on its surface that is labeled axis. Still farther along the ray is a single blue double headed arrow oriented vertically that is labeled E and direction of polarization.
A polarizing filter has a polarization axis that acts as a slit passing through electric fields parallel to its direction. The direction of polarization of an EM wave is defined to be the direction of its electric field.

[link] shows the effect of two polarizing filters on originally unpolarized light. The first filter polarizes the light along its axis. When the axes of the first and second filters are aligned (parallel), then all of the polarized light passed by the first filter is also passed by the second. If the second polarizing filter is rotated, only the component of the light parallel to the second filter’s axis is passed. When the axes are perpendicular, no light is passed by the second.

Only the component of the EM wave parallel to the axis of a filter is passed. Let us call the angle between the direction of polarization and the axis of a filter θ size 12{θ} {} . If the electric field has an amplitude E size 12{E} {} , then the transmitted part of the wave has an amplitude E cos θ size 12{E"cos"θ} {} (see [link] ). Since the intensity of a wave is proportional to its amplitude squared, the intensity I size 12{I} {} of the transmitted wave is related to the incident wave by

I = I 0 cos 2 θ , size 12{I=I rSub { size 8{0} } "cos" rSup { size 8{2} } θ,} {}

where I 0 size 12{I rSub { size 8{0} } } {} is the intensity of the polarized wave before passing through the filter. (The above equation is known as Malus’s law.)

This figure has four subfigures. The first three are schematics and the last is a photograph. The first schematic looks much as in the previous figure, except that there is a second polarizing filter on the axis after the first one. The second polarizing filter has its lines aligned parallel to those of the first polarizing filter (i e, vertical). The vertical double headed arrow labeled E that emerges from the first polarizing filter also passes through the second polarizing filter. The next schematic is similar to the first, except that the second polarizing filter is rotated at forty five degrees with respect to the first polarizing filter. The double headed arrow that emerges from this second filter is also oriented at this same angle. It is also noticeably shorter than the other double headed arrows. The third schematic shows the same situation again, except that the second polarizing filter is now rotated ninety degrees with respect to the first polarizing filter. This time, there is no double headed arrow at all after the second polarizing filter. Finally, the last subfigure shows a photo of three circular optical filters placed over a bright colorful pattern. Two of these filters are place next to each other and the third is placed on top of the other two so that the center of the third is at the point where the edges of the two filters underneath touch. Some light passes through where the upper filter overlaps the left-hand underneath filter. Where the upper filter overlaps the right-hand lower filter, no light passes through.
The effect of rotating two polarizing filters, where the first polarizes the light. (a) All of the polarized light is passed by the second polarizing filter, because its axis is parallel to the first. (b) As the second is rotated, only part of the light is passed. (c) When the second is perpendicular to the first, no light is passed. (d) In this photograph, a polarizing filter is placed above two others. Its axis is perpendicular to the filter on the right (dark area) and parallel to the filter on the left (lighter area). (credit: P.P. Urone)
This schematic is another variation of the schematic first introduced two figures prior. To the left of the vertically oriented polarizing filter is a double headed blue arrow oriented in the plane perpendicular to the propagation direction and at an angle theta with the vertical. After the polarizing filter a smaller vertical double headed arrow appears, which is labeled E cosine theta.
A polarizing filter transmits only the component of the wave parallel to its axis, E cos θ size 12{E"cos"θ} {} , reducing the intensity of any light not polarized parallel to its axis.

Calculating intensity reduction by a polarizing filter

What angle is needed between the direction of polarized light and the axis of a polarizing filter to reduce its intensity by 90 . 0% size 12{"90" "." 0%} {} ?

Strategy

When the intensity is reduced by 90 . 0% size 12{"90" "." 0%} {} , it is 10 . 0% or 0.100 times its original value. That is, I = 0 . 100 I 0 . Using this information, the equation I = I 0 cos 2 θ size 12{I=I rSub { size 8{0} } "cos" rSup { size 8{2} } θ} {} can be used to solve for the needed angle.

Solution

Solving the equation I = I 0 cos 2 θ size 12{I=I rSub { size 8{0} } "cos" rSup { size 8{2} } θ} {} for cos θ size 12{"cos"θ} {} and substituting with the relationship between I size 12{I} {} and I 0 size 12{I rSub { size 8{0} } } {} gives

cos θ = I I 0 = 0 . 100 I 0 I 0 = 0 . 3162. size 12{"cos"θ= sqrt { { {I} over {I rSub { size 8{0} } } } } = sqrt { { {0 "." "100"I rSub { size 8{0} } } over {I rSub { size 8{0} } } } } =0 "." "316"} {}

Solving for θ size 12{θ} {} yields

θ = cos 1 0 . 3162 = 71 . 6º. size 12{θ="cos" rSup { size 8{ - 1} } 0 "." "316"="71" "." 6°} {}

Discussion

A fairly large angle between the direction of polarization and the filter axis is needed to reduce the intensity to 10 . 0% size 12{"10" "." 0%} {} of its original value. This seems reasonable based on experimenting with polarizing films. It is interesting that, at an angle of 45º size 12{"45"°} {} , the intensity is reduced to 50% size 12{"50"%} {} of its original value (as you will show in this section’s Problems&Exercises). Note that 71 . size 12{"71" "." 6°} {} is 18 . size 12{"18" "." 4°} {} from reducing the intensity to zero, and that at an angle of 18 . size 12{"18" "." 4°} {} the intensity is reduced to 90 . 0% size 12{"90" "." 0%} {} of its original value (as you will also show in Problems&Exercises), giving evidence of symmetry.

Questions & Answers

A golfer on a fairway is 70 m away from the green, which sits below the level of the fairway by 20 m. If the golfer hits the ball at an angle of 40° with an initial speed of 20 m/s, how close to the green does she come?
Aislinn Reply
cm
tijani
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John Reply
what is physics
Siyaka Reply
A mouse of mass 200 g falls 100 m down a vertical mine shaft and lands at the bottom with a speed of 8.0 m/s. During its fall, how much work is done on the mouse by air resistance
Jude Reply
Can you compute that for me. Ty
Jude
what is the dimension formula of energy?
David Reply
what is viscosity?
David
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emma Reply
what is chemistry
Youesf Reply
what is inorganic
emma
Chemistry is a branch of science that deals with the study of matter,it composition,it structure and the changes it undergoes
Adjei
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Adjanou
chemistry could also be understood like the sexual attraction/repulsion of the male and female elements. the reaction varies depending on the energy differences of each given gender. + masculine -female.
Pedro
A ball is thrown straight up.it passes a 2.0m high window 7.50 m off the ground on it path up and takes 1.30 s to go past the window.what was the ball initial velocity
Krampah Reply
2. A sled plus passenger with total mass 50 kg is pulled 20 m across the snow (0.20) at constant velocity by a force directed 25° above the horizontal. Calculate (a) the work of the applied force, (b) the work of friction, and (c) the total work.
Sahid Reply
you have been hired as an espert witness in a court case involving an automobile accident. the accident involved car A of mass 1500kg which crashed into stationary car B of mass 1100kg. the driver of car A applied his brakes 15 m before he skidded and crashed into car B. after the collision, car A s
Samuel Reply
can someone explain to me, an ignorant high school student, why the trend of the graph doesn't follow the fact that the higher frequency a sound wave is, the more power it is, hence, making me think the phons output would follow this general trend?
Joseph Reply
Nevermind i just realied that the graph is the phons output for a person with normal hearing and not just the phons output of the sound waves power, I should read the entire thing next time
Joseph
Follow up question, does anyone know where I can find a graph that accuretly depicts the actual relative "power" output of sound over its frequency instead of just humans hearing
Joseph
"Generation of electrical energy from sound energy | IEEE Conference Publication | IEEE Xplore" ***ieeexplore.ieee.org/document/7150687?reload=true
Ryan
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Maurice Reply
what are the types of wave
Maurice
answer
Magreth
progressive wave
Magreth
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Muhammad Reply
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Mohammed
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Mujahid
A string is 3.00 m long with a mass of 5.00 g. The string is held taut with a tension of 500.00 N applied to the string. A pulse is sent down the string. How long does it take the pulse to travel the 3.00 m of the string?
yasuo Reply
Who can show me the full solution in this problem?
Reofrir Reply
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Source:  OpenStax, Yupparaj english program physics corresponding to thai physics book #3. OpenStax CNX. May 19, 2014 Download for free at http://legacy.cnx.org/content/col11657/1.1
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