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Physics 212 Lecture 24 Physics 212 Lecture 24 Electricity & Magnetism Lecture 24, Slide 1 Your Comments Why do we want to polarize light? What is polarized light used for? I feel like after the polarization lecture the Professor laughs and goes tell his friends, "I ran out of things to teach today so I made some stuff up and the students totally bought it." I really wish you would explain the new right hand rule. I cant make it work in my mind I can't wait to see what demos are going to happen in class!!! This topic looks like so much fun!!!! With E related to B by E=cB where c=(u0e0)^-0.5, does the ratio between E and B change when light passes through some material m for which em =/= e0? I feel like if specific examples of homework were done for us it would help more, instead of vague general explanations, which of course help with understanding the theory behind the material. THIS IS SO COOL! Could you explain what polarization looks like? The lines that are drawn through the polarizers symbolize what? Are they supposed to be slits in which light is let through? Real talk? The Law of Malus is the most metal name for a scientific concept ever devised. Just say it in a deep, commanding voice, "DESPAIR AT THE LAW OF MALUS." Awesome! Electricity & Magnetism Lecture 24, Slide 2 Linearly Polarized Light So far we have considered plane waves that look like this: From now on just draw E and remember that B is still there: Electricity & Magnetism Lecture 24, Slide 3 Linear Polarization “I was a bit confused by the introduction of the "e-hat" vector (as in its purpose/usefulness)” Electricity & Magnetism Lecture 24, Slide 4 Polarizer The molecular structure of a polarizer causes the component of the E field perpendicular to the Transmission Axis to be absorbed. Electricity & Magnetism Lecture 24, Slide 5 Clicker Question The molecular structure of a polarizer causes the component of the E field perpendicular to the Transmission Axis to be absorbed. Eo Suppose we have a beam traveling in the + z - direction. At t = 0 and z = 0, the electric field is aligned along the positive y x - axis and has a magnitude equal to Eo z What is the component of Eo along a direction in the x - y plane that makes an angle of q with respect to the x - axis? Eo q A) Eosinq B) Eocosq C) 0 D) Eo/sinq E) Eo/cosq Electricity & Magnetism Lecture 24, Slide 6 Linear Polarizers “I can't believe your teaching us the law of "Malus"(Malice). I thought malice was to be avoided?” Electricity & Magnetism Lecture 24, Slide 7 CheckPoint 1a An unpolarized EM wave is incident on two orthogonal polarizers. Two Polarizers What percentage of the intensity gets through both polarizers? A. 50% The secondB. 25% polarizer is orthogonalC. 0% to the first No light will come through. cos(90o) = 0 Electricity & Magnetism Lecture 24, Slide 8 CheckPoint 1b An unpolarized EM wave is incident on two orthogonal polarizers. Two Polarizers Is it possible to increase this percentage by inserting another Polarizer between the original two? A. Yes B. No DEMO Electricity & Magnetism Lecture 24, Slide 9 Circularly Polarized Light There is no reason that f has to be the same for Ex and Ey: Making fx different from fy causes circular or elliptical polarization: Example: At t = 0 f -f = 90 = x y 2 q = 45 = / 4 E E = 0 coskz-t x 2 E E=-0 sin kz t RCP y 2 Electricity & Magnetism Lecture 24, Slide 10 Quarter Waveplates Q: How do we change the relative phase between Ex and Ey? A: Birefringence By picking the right thickness we can change the relative phase by exactly 90o. This changes linear to Right circular polarization hand rule and is called a quarter wave plate Electricity & Magnetism Lecture 24, Slide 11 Intensity does not change! “talk something about intensity” NOTE: No Intensity is lost passing through the QWP ! BEFORE QWP: ˆ ˆ i + j I = c E2 = c E2 + E2 E = Eo sin(kz-t) o o x y 2 E2 E2 1 = c o + o sin2 (kz-t) = c E2 o 2 2 o o 2 AFTER QWP: E E = o iˆcos(kz-t) + ˆjsin(kz-t) I = c E2 = c E2 + E2 2 o o x y E2 = c o cos2 (kz-t) + sin2 (kz-t) o 2 E2 E2 = c o 1 = c o THE SAME! o 2 o 2 Electricity & Magnetism Lecture 24, Slide 12 Right or Left Circularly Polarized E Ey Ex Ey Ex A linearly polarized EM wave is incident on a quarter-wave plate as shown above. The resulting wave is A) Right Circularly Polarized Curve fingers from slow to fast, B) Left Circularly Polarized thumb must be direction of C) Linearly Polarized propagation. Electricity & Magnetism Lecture 24, Slide 14 Circular Light on Linear Polarizer Q: What happens when circularly polarized light is put through a polarizer along the y (or x) axis ? A) I = 0 B) I = ½ I0 C) I = I0 2 I = 0c E 2 2 = 0c Ex + EXy 2 1 1 2 E = 0cE0 = c 0 cos2 (kz-t) 2 2 0 2 Half of before 1/2 Electricity & Magnetism Lecture 24, Slide 15 CheckPoint 2a Identical linearly polarized light at 45o from the y-axis and propagating along the z axis is incident on two different objects. In Case A the light intercepts a linear polarizer with polarization alongA the y-axis In Case B, the light Bintercepts a quarter wave plate with vast axis along the y-axis. Case A Case B Compare the intensities of the light waves after transmission. A. IA < IB B. IA = IB C. IA > IB Case A: Case B: Ex is absorbed (Ex ,Ey) phase changed 2 o I A = I0 cos (45 ) 1 I = I I A = 2 I0 B 0 Electricity & Magnetism Lecture 24, Slide 16 Identical linearly polarized light at 45o from the y-axis and propagating along the z axis is incident on two different objects.CheckPoint In Case A the light intercepts2b a linear polarizer with polarization along the y-axis In Case B, the light intercepts a quarter wave plate with vast axis along the y-axis. Case AA Case BB What is the polarization of the light wave in Case B after it passes through the quarter wave plate?. A. linearly polarized B. left circularly polarized C. right circularly polarized D. undefined RCP 1/4 l Z Electricity & Magnetism Lecture 24, Slide 19 CheckPoint 2c Identical linearly polarized light at 45o from the y-axis and propagating along the z axis is incident on two different objects. In Case A the light intercepts a linear polarizer with polarization along the y-axis In Case B, the light intercepts a quarter wave plate with vast axis along the y-axis. Case A Case B If the thickness of the quarter-wave plate in Case B is doubled, what is the polarization of the wave after passing through the wave plate? A. linearly polarized B. circularly polarized C. undefined ½ l Z Z Electricity & Magnetism Lecture 24, Slide 20 Executive Summary: Polarizers & QW Plates: Polarized Light Circularly or Un-polarized Light Birefringence RCP E E= 0 cos( kx ) x 2 E E= 0 sin( kx ) y 2 Electricity & Magnetism Lecture 24, Slide 21 Calculation Light is incident on two linear polarizers and a quarter wave plate (QWP) as shown. What is the intensity I3 in terms of I1? 45o fast y x 60o I1 I2 z I3 Conceptual Analysis Linear Polarizers: absorbs E field component perpendicular to TA Quarter Wave Plates: Shifts phase of E field components in fast-slow directions Strategic Analysis Determine state of polarization and intensity reduction after each object Multiply individual intensity reductions to get final reduction. Electricity & Magnetism Lecture 24, Slide 23 Calculation Light is incident on two linear polarizers and a quarter wave plate (QWP) as shown. fast y 45o E RCP x 1 Ex E y 60o I1 l / 4 I 2 z I3 What is the polarization of the light after the QWP? y y A) LCP B) RCP C) x D) x E) un-polarized Light incident on QWP is linearly Light will be circularly polarized at 45o to fast axis polarized after QWP LCP or RCP? Easiest way: Curl fingers of RH back to front Right Hand Rule: Thumb points in dir of propagation RCP if right hand polarized. Electricity & Magnetism Lecture 24, Slide 24 Calculation Light is incident on two linear polarizers and a quarter wave plate (QWP) as shown. fast y 45o E RCP x 1 Ex E y 60o I1 l / 4 I 2 z I3 What is the intensity I2 of the light after the QWP? A) I2 = I1 B) I2 = ½ I1 C) I2 = ¼ I1 Before: No absorption: Just a phase change! After: E1 E Ex = sinkz-t E = 1 cos kz-t 2 2 2 x I = 0c Ex + Ey 2 E 1 E1 Ey = sinkz-t E = coskz-t 2 Same before & after! y 2 Electricity & Magnetism Lecture 24, Slide 25 Calculation Light is incident on two linear polarizers and a quarter wave plate (QWP) as shown. fast y 45o E RCP x 1 Ex E y 60o E3 I1 l / 4 I = I 2 1 z I3 What is the polarization of the light after the 60o polarizer? y y 60o 60o A) LCP B) RCP C) x D) x E) un-polarized Absorption: only passes components of E parallel to TA (q = 60o) E y 3 E = E sinq + E cosq E1 E3 3 x y E = sin(kz-t +q) 3 2 60o E E = 1 cos(kz-t)sinq + sin(kz-t)cosq 3 2 Ex Electricity & Magnetism Lecture 24, Slide 26 Calculation Light is incident on two linear polarizers and a quarter wave plate (QWP) as shown.
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