2. Waves can be represented by simple harmonic motion

3. Standing wave y = Asin(kx − ωt) + Asin(kx + ωt)

4. The amplitude of a wave is a measure of the maximum disturbance in the medium during one wave cycle. (the maximum distance from the highest point of the crest to the equilibrium). The wavelength (denoted as λ) is the distance between two sequential crests (or troughs). This generally has the unit of meters. A wavenumber Period Phase velocity:

5. Electromagnetic waves

7. Light as a Wave (1) Light waves are characterized by a wavelength  and a frequency f. f = c/ c = 300,000 km/s = 3*10 8 m/s f and are related through

8. The Electromagnetic Spectrum Need satellites to observe Wavelength Frequency High flying air planes or satellites

9. Dual, wave-particle nature of light 1 eV = 1.6x10 -19 J c = 3x10 8 m/s 1 Angstrom = 10 -10 m Speed of light in matter: c m = c/n, where n is refractive index Note: n is a function of

10. Light as a Wave (2) Wavelengths of light are measured in units of nanometers (nm) or Ångström (Å): 1 nm = 10 -9 m 1 Å = 10 -10 m = 0.1 nm Visible light has wavelengths between 4000 Å and 7000 Å (= 400 – 700 nm).

11. Light as Particles Light can also appear as particles, called photons (explains, e.g., photoelectric effect). A photon has a specific energy E, proportional to the frequency f: E = h*f h = 6.626x10 -34 J*s is the Planck constant. The energy of a photon does not depend on the intensity of the light!!!

12. Maxwell’s Equations

13. Information Age The cost of the transmission, storage and processing of data has been decreasing extremely fast Information is available anytime, any place, and for everyone Information and knowledge became a capital asset All of this became possible because of several revolutionary ideas

14. Telecommunications

15. Samuel Morse's telegraph key, 1844. Today's information age began with the telegraph. It was the first instrument to transform information into electrical signal and transmit it reliably over long distances. Alexander Graham Bell’s commercial telephone from 1877. How it all started …

16. Speaking into the handset's transmitter or microphone makes its diaphragm vibrate. This varies the electric current, causing the receiver's diaphragm to vibrate. This duplicates the original sound. Telephone connection requires a dedicated wire line; Only one communication is possible at a time

17. How many channels are possible? How many signals can be transmitted at the same time?? Radio: communication through radio waves 1895 Alexander Popov Guglielmo Marconi www.nrao.edu Frequency measured in Hertz 1 Hz = 1 cycle/second 1 kHz = 1000 cycles/second

18. Radio stations have to broadcast at different carrier frequencies to avoid cross-talk Range of frequencies (Bandwidth) needs to be at least 20 kHz for each station Human ear: 10 Hz-20 kHz Frequencies of different stations should be at least 20 kHz apart

19. Higher carrier frequencies Wider bandwidth Higher data rate, more channels Need more channels? Need higher speed? Use higher frequencies for transmission! Using light? Optical frequencies ~ 10 14 Hz !

20. How can we send light over long distances? Air? Only within line of sight; High absorption and scattering, especially when it rains Are there any “light wires” (optical waveguides)? Copper wire? High absorption, narrow bandwidth 300 MHz Glass? Window glass absorbs 90% of light after 1 m. Only 1% transmission after 2 meters. Sand?!

21. Transmisson 95.5% of power after 1 km 1% of power after 100 km: need amplifiers and repeaters Total bandwidth ~ 100,000 GHz!! Ultra-low absorption in silica glasses Silica (Silicon dioxide) is sand – the most abundant mineral on Earth Predicted 1965, in first low-loss fiber in 1970

22. Total internal reflection! n 1 > n 2 How to trap light with transparent material?? Light coming from more refractive to less refractive medium experiences total reflection – get trapped there!

23. No charges, no real currents Wave equation

24. k is a wave number, is a wave length, T is the period Velocity of propagation

25. Coulomb’s Law Charge Conservation of electric charge Charge is conserved: in any isolated system, the total charge cannot change. If it does change, then the system is not isolated: charge either went somewhere or came in from somewhere is the permittivity of free space

26. Charge Let’s denote the force that exerts on as and force exerted by on as ; r is the distance between charges. (Newton’s third law works!) Like charges repel; opposites attract

27. Exercise: If two electrons are placed meters apart, what is the magnitude of the Coulomb force between them? Compare this to the gravitational force between them. Solution: The magnitude of electric force The magnitude of gravitational force (no matter what the separation is) r

28. Gauss’s Law A conducting sphere, conducting shell, insulating sphere, shell …..

29. d + + + + + + a - - - (the total field at any point between the plates) Two parallel conducting plates

30. Capacitors Consider two large metal plates which are parallel to each other and separated by a distance small compared with their width. Area A The field between plates is L

31. The capacitance is:

32. Capacitors in series: Capacitors in parallel:

33. Current, Ohm’s Law, Etc.

34. Current Density Consider current flowing in a homogeneous wire with cross sectional area A.

35. For steady state situation Circuits will be included!

36. Joule’s Law

37. The force on a charge q moving with a velocity If the magnitude of the force

38. The angular velocity

39. Using Crossed and Fields Velocity selector independent of the mass of the particle!

40. Ampere’s Law The field produced by an infinite wire

41. Biot-Savart Law Infinitesimally small element of a current carrying wire produces an infinitesimally small magnetic field (Also called Ampere’s principle) is called permeability of free space

42. Force exerted on a current carrying wire For a straight, finite wire of length and uniform magnetic field

43. Faraday’s Law of Induction The induced EMF in a closed loop equals the negative of the time rate of change of magnetic flux through the loop

44. There can be EMF produced in a number of ways: A time varying magnetic field An area whose size is varying A time varying angle between and Any combination of the above

45. R From Faraday’s law: a time varying flux through a circuit will induce an EMF in the circuit. If the circuit consists only of a loop of wire with one resistor, with resistance R, a current Which way? Lenz’s Law: if a current is induced by some change, the direction of the current is such that it opposes the change.

46. A Simple Generator

47. Faraday’s Law is used to obtain differential equations for some simple circuits. Self-inductance L

48. Displacement current

49. Thank you for a great semester!