Phys 102 – Lecture 16 Electromagnetic wave energy & polarization.

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Presentation transcript:

Phys 102 – Lecture 16 Electromagnetic wave energy & polarization

Today we will... Learn about properties of electromagnetic waves Energy density & intensity Polarization – linear, circular, unpolarized Apply those concepts Linear polarizers Optical activity Circular dichroism

E & B field energy density There is energy stored in an E & B field B Solenoid A d Parallel plate capacitor E Recall Lect. 6 Volume containing E field It is convenient to define energy density = energy per volume [J/m3] These expressions are correct for any E & B field in a vacuum

EM wave energy There is energy stored in an EM wave in oscillating E & B fields E0 B0 B(t) E(t) Since E and B oscillate, we measure the average energy density E & B field amplitudes Recall that

EM wave intensity A source of light emits EM energy at a rate given by the power P: Units: W Same energy flows through surfaces at larger distances, but spread over a larger surface area A. Energy flowing through surface in time Δt: It is useful to define intensity: Units: W/m2 Intensity corresponds to “brightness” of light

ACT: EM wave intensity IP is the light intensity at a point P a distance r from a point source, a 60 W light bulb. (Assume all electric power goes into EM wave) IP r ? 2r What is the light intensity at a distance 2r? 2IP IP IP/2 IP/4

Calculation: EM power A light bulb emits an average 60 W of power. Calculate Erms & Brms at a distance r = 2 m from bulb. (Assume all electric power goes into EM wave) r = 2 m By energy conservation, power emitted = power through spherical surface at r = 2 m

CheckPoint 1.1–1.7 Longitudinal waves: oscillations are || to direction or propagation Transverse waves: oscillations are  to direction of propagation λ DEMO λ All EM waves! DEMO 353: Slinky http://www.youtube.com/watch?v=5CAYNTBrczo Ex: Sound Ex: Light Radio waves X-rays Microwaves Water waves “The wave” Compressed air Expanded air E B

Polarization EM waves are transverse and have polarization – by convention, the direction of the E field oscillation x z Linear E B y x z Ex: “Vertical” polarization Circular E B y x z x z Ex: “Left” circular polarization Unpolarized – direction is random For convenience we will stop showing the B field

Linear polarizers Linear polarizers consist of || metal lines that absorb || E field. Transmission axis (TA) is defined in direction that E field passes TA E E  TA: no light passes TA E E || TA: light passes What happens for other angles between polarization and TA?

Law of Malus Given angle θ between TA and polarization of incident EM wave: Einc θ Einc θ Etrans TA TA Component of E field  to TA axis is absorbed: θ TA θ 360 180 Itrans Iinc Since Light emerges with polarization || to TA axis

ACT: polarizer A vertically polarized EM wave passes through a linear polarizer with TA at 45° Einc TA What is the direction of the B field after the polarizer? B. C. D. What is the magnitude?

Calculation: unpolarized light Unpolarized light is incident on a linear polarizer. What is the transmitted intensity? TA Einc Etrans Unpolarized light has an equal mixture of all possible θ’s θ 360 180 Itrans Iinc average over all θ: Iinc/2 Light emerges with polarization || to TA axis

ACT: CheckPoint 2.1 Unpolarized light passes through a linear polarizer with a vertical TA. I0 TA What is the intensity of light when it emerges? zero 1/2 what it was before 1/4 what it was before 1/3 what it was before

ACT: CheckPoint 2.2 Now the light that emerged from the previous polarizer passes through a second linear polarizer with a horizontal TA. 1 2 I0 TA TA What is the intensity of light when it emerges? zero 1/2 what it was before 1/4 what it was before 1/3 what it was before

ACT: 3 polarizers Now suppose we add a third polarizer between the two outer polarizers. The polarizer TA is tilted from vertical. 1 TA 3 2 Demo I0 TA TA What is the intensity of the light that emerges? DEMO zero, same as before more than what it was before need more information

Calculation: 3 polarizers 1 3 2 I0 TA TA TA

Chirality & optical activity Many organic molecules are chiral – they have “handedness” L-alanine D-alanine (unnatural enantiometer) Chiral molecules rotate linearly polarized light – optical activity “Dextrorotary” CW rotation “Levorotary” CCW rotation DEMO

Circular dichroism Chiral molecules also absorb left vs. right circularly polarized light differently Circular dichroism (CD) measures difference in absorption Tool to distinguish chiral features in biomolecules α-helix (right-handed helix) CD spectra

ACT: Law of Malus A θ01 = 60° B θ01 = 60° I0 I0 2 2 TA TA TA TA Compare the light emerging from the two polarizers in A and B: A. I2A > I2B B. I2A = I2B C. I2A < I2B

Summary of today’s lecture Electromagnetic waves Carry energy in E and B fields – energy density & intensity Are transverse & polarized – linear, circular, unpolarized Applications Linear polarizers – Law of Malus Optical activity Circular dichroism