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Three models of light PDF

94 Pages·2014·10.04 MB·English
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Light Light: Three models • Newton’s particle model (rays) – Models light as bits of energy traveling very fast in straight lines. • Huygens’s/Maxwell wave model – Models light at waves (transverse EM waves). Color determined by frequency, intensity by square of a total oscillating amplitude. • Einstein’s photon model – Models light as “wavicles” == quantum particles whose energy is determined by frequency and that can interfere with themselves. 4/23/2014 PHYS132 2 Venn Diagram Quantum Electrodynamics Physical Optics (Wave model) Geometric Optics (Ray model) Einstein’s photon model 4/23/2014 PHYS132 3 Modeling in Biology Are there examples in biology where you also need different models ? Each model highlights different properties of the protein - Hydrophobic character - Folding property 4/23/2014 PHYS132 4 Reason for multiple models • Each “model” of light highlights a particular characteristic of light (just like each model of a protein highlights a particular aspect of what proteins are and how they work) 4/23/2014 PHYS132 5 Light: Purpose of the three models • Newton’s particle model (rays) – Models how light interacts with mirrors and lenses • Huygens’s/Maxwell wave model – Models cancellation and interference • Einstein’s photon model – Models absorption and emission of light 4/23/2014 PHYS132 6 The Ray Model 4/23/2014 PHYS132 7 Classical Electromagnetism - Maxwell’s Equations Everything in models (1) and (2) is contained in Maxwell’s Equations Charge density 𝜌 𝛻 � 𝐄 = 𝜖0 𝜕𝐁 𝛻 × 𝐄 = − 𝜕𝜕 𝛻 � 𝐁 = 0 𝜕𝐄 𝛻 × 𝐁 = 𝜇0 𝑱⃑ + 𝜖0 𝜕𝜕 Current density You are not expected to know these. Just know they exist. 4/23/2014 PHYS132 8 Electromagnetic Waves are one type of solution to Maxwell’s equations 4/23/2014 PHYS132 9 Special Case Sinusoidal Waves E y (x, t) = f+ (x - vemt) = E0 cos[k(x - vemt)] Wavenumber and wavelength E (x, t) y 2𝜋 E 0 𝑘 = λ 2𝜋 λ = 𝑘 - E 0 These two contain the same information 4/23/2014 PHYS132 10

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