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UW-Madison PHYSICS 208 - LECTURE NOTES

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Physics 208, Lecture 22 Today’s Topics  Electromagnetic Waves (EM Waves)  Review: Waves and Wave Equation  Maxwell’s Equations  Propagation of E and B  Energy Carried by EM Wave, Poynting Vector  Momentum Carried by EM Wave  Spectrum of EM wave. 1Maxwell Equations € E • dA =qε0∫ € E • d = −dΦBdt∫€ F = qE + qv × B € B• d =µ0I +ε0µ0dΦEdt∫€ B• dA = 0∫Gauss’s Law/ Coulomb’s Law Faraday’s Law Gauss’s Law of Magnetism, no magnetic charge Ampere Maxwell Law Also, Lorentz force Law  These are the foundations of electromagnetism 2EM Fields in Space  Maxwell equations when there is no charge and current: ∫=• 0AE d € E • d = −dΦBdt∫ € B• d =ε0µ0dΦEdt∫∫=• 0AB dtBxEzy∂∂−=∂∂tExByz∂∂−=∂∂00εµdifferential forms: (single polarization) x y z 220022tExEyy∂∂=∂∂εµ220022tBxBzz∂∂=∂∂εµE B 3Linear Wave Equation  Linear wave equation 222221tyvxy∂∂=∂∂certain physical quantity Wave speed  Sinusoidal wave y = Asin2πλx − 2πft +ϕ⎛⎝⎜⎞⎠⎟A:Amplitude f: frequency φ:Phase General wave: sum of sinusoidal waves v=λf k=2π/λ$ω=2πf λ:wavelength 4Electromagnetic Waves  EM wave equations:  Plane wave solutions: E= Emaxsin(kx-ωt+φ) B= Bmaxsin(kx-ωt+φ)  Properties:  No medium is necessary.  E and B are normal to each other  E and B are in phase  Direction of wave is normal to both E and B (EM waves are transverse waves)  Speed of EM wave:  E/B = Emax/Bmax=c  Transverse wave: two polarizations possible same φ, set to be 0 smc /109972.21800×==εµx y z E B c 5The EM Wave x y z E B c Two polarizations possible 6Wavelength and Frequency  Because of the wave equation the wavelength of and frequency of a EM wave in vacuum are related by:  Example: Determine the wavelength of an EM wave of frequency 50 MHz in free space € λf = c = 3⋅108m / s€ λ=cf=3⋅108m / s50 MHz=3⋅108m / s5 ⋅107s−1= 6m7Energy Carried By EM Waves  Recall: energy densities uE= ½ ε0E2, uB= ½ B2/µ0  For a EM wave, at any time/location, uE = ½ ε0E2 = ½ B2/µ0 =uB (using E/B=c)  In an electromagnetic wave, the energies carried by electric field and magnetic field are always the same.  Total energy stored (per unit of volume): u=uE+uB = ε0E2 = B2/µ0  Power transmitted per unit of area is equal to uc in the direction of wave  Averaging over time: uav= ½ ε0Emax2 = ½ Bmax2/µ0 , uavc = I (intensity) x y z E B 8The Poynting Vector  The rate of flow of energy in an em wave is described by a vector, S , called the Poynting vector  The Poynting vector is defined as  Its direction is the direction of propagation  This is time dependent  Its magnitude varies in time  Its magnitude reaches a maximum at the same instant as E and B €  S ≡1µ0 E × B Power per unit of area € I = Sav9Momentum Carried By EM Waves  EM waves: momentum = energy/c  Radiation Pressure (P): A ΔX=cΔt S 100% absorption Δp = p  P= S/c 100% reflection Δp = 2p  P= 2S/c € Δp =ΔUc=uAcΔtc= uAΔt€ Δp = 2ΔUc= 2uAcΔtc= 2uAΔtChange of momentum in 100% absorption Change of momentum in 100% reflection € P =FA=ΔpΔtA= u =Sc10Example: Solar Energy  The average intensity of the EM radiation from the Sun on Earth is S ~ 103 W/m2  What is the average radiation pressure for 100% absorption:  What is the force exerted by EM radiation by the Sun on a surface of 1 m2 € P =Sc=103W m23⋅108ms= 3.3⋅10−6N m2€ F = PA = 3.3⋅10−6N m2⋅1m2= 3.3⋅10−6N11Antennas  Antennas are essentially arrangement of conductors for transmitting and receiving radio waves.  Parameters: gain, impedance, frequency, orientation, polarization, etc. half-wave antenna loop λ/4$λ/4$maximum strength microstrip 12Spectrum of EM Waves λf=c f (Hz) λ$VHF: 30-300 MHz UHF: 300 MHz -3.0 GHz Cell phone: 800/900/1800/1900 MHz Wifi: 2.4 GHz & 5 GHz Microwave Oven: 2.4 GHz Wireless phone: 2.4/5.8 GHz MHz GHz


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UW-Madison PHYSICS 208 - LECTURE NOTES

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Lect 11

Lect 11

19 pages

EM Waves

EM Waves

23 pages

Exam 3

Exam 3

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