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1 Photoelectricity Classically, light is treated as EM wave according to Maxwell equation However, in a few types of experiments, light behave in ways.

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Presentation on theme: "1 Photoelectricity Classically, light is treated as EM wave according to Maxwell equation However, in a few types of experiments, light behave in ways."— Presentation transcript:

1 1 Photoelectricity Classically, light is treated as EM wave according to Maxwell equation However, in a few types of experiments, light behave in ways that is not consistent with the wave picture In these experiments, light behave like particle instead So, is light particle or wave? (recall that wave and particle are two mutually exclusive attributes of existence) This is a paradox that we will discuss in the rest of the course – wave particle duality

2 2 Photoelectric effect

3 3 Photoelectrons are ejected from a metal surface when hit by a monochromatic light, frequency The photoelectrons are attracted to the collecting anode (positive) by potential difference applied on the anode and detected as electric current by the external circuits

4 4 -0-0 K max = e  0

5 5 Features of the experimental result When the external potential difference V = 0, the current is not zero because the photoelectrons carry some kinetic energy, K K range from 0 to a maximal value, K max As V becomes more and more positive, there are more electrons attracted towards the anode within a given time interval. Hence the current, I, increases with V Saturation of I will be achieved when all of the ejected electron are immediately attracted towards the anode once they are kicked out from the metal plates

6 6 On the other direction, when V becomes more negative, the photocurrent detected decreases in magnitude because the electrons are now moving against the potential K max can be measured. It is given by e  0, where  0, is the value of V when the current flowing in the external circuit = 0 (why?)  0 is called the ‘stopping potential’

7 7 One finds that, at constant frequency, the same maximal kinetic energy of the photoelectrons is the same (  0 ) when the intensity of light increases

8 8 Another feature: cutoff frequency One can also detect the stopping potential at different frequency (for a given material) There exist a cut-off frequency, 0, below which no PE effect occurs (no matter how intense is the radiation shined on the metal surface) For different material, the cut-off frequency is different

9 9

10 10 Puzzle one: If light were wave, the energy carried by the radiation will increases as the intensity of the monochromatic light increases Hence we would also expect K max of the electron to increase as the intensity of radiation increases (because K.E. of the photoelectron must come from the energy of the radiation) YET THE OBSERVATION IS OTHERWISE.

11 11 Puzzle two: Existence of a characteristic cut-off frequency, 0. Wave theory predicts that photoelectric effect should occur for any frequency as long as the light is intense enough to give the energy to eject the photoelectrons. No cut-off frequency is predicted.

12 12 Puzzle three No detection time lag measured. Classical wave theory needs a time lag between the instance the light impinge on the surface with the instance the photoelectrons being ejected. Energy needs to be accumulated for the wave front, at a rate proportional to, before it has enough energy to eject photoelectrons. But, in the PE experiments, photoelectricity is almost immediate

13 13 Cartoon analogy: in the wave picture, accumulating the energy required to eject an photoelectron from an atom is analogous to filling up a tank with water from a pipe until the tank is full. One must wait for certain length of time (time lag) before the tank can be filled up with water at a give rate. The total water filled is analogous to the total energy absorbed by electrons before they are ejected from the metal surface at Electron spills out from the tank when the water is filled up gradually after some ‘time lag’ Water from the pipe fills up the tank at some constant rate

14 14 Example: Wave theory and the time delay problem: A potassium foil is placed at a distance r = 3.5 m from a light source whose output power P is 1.0 W. How long would it take for the foil to soak up enough energy (=1.8 eV) from the beam to eject an electron? Assume that the ejected electron collected the energy from a circular area of the foil whose radius is 5.3 x m

15 15 r=3.5m Area of sphere, A =  r 2 Area of the surface presented by an atom, a =  r b 2, where r b = 0.5 Angstrom Energy from the bulb, P 0 = 1 W (or joule per second) Energy absorbed by a is  = (a/A) x P 0 = (  r b 2 /  r 2 ) x 1 Watt = 5.7x Watt

16 16 Time taken for a to absorb 1.8 eV is simply 1.8 x 1.6 x J /  5000 s = 1.4 h!!! In PE, the photoelectrons are ejected almost immediately but not 1.4 hour later This shows that the wave model used to calculate the time lag in this example fails to account for the almost instantaneous ejection of photoelectron in the PE experiment

17 17 Einstein’s quantum theory of the photoelectricity (1905) A Noble-prize winning theory (1905) To explain PE, Einstein postulates that the radiant energy of light is quantized into concentrated bundle. The discrete entity that carries the energy of the radiant energy is called photon Or, in quantum physics jargon, we say “photon is the quantum of light” Wave behaviour of light is a result of collective behaviour of very large numbers of photons

18 18 Flux of radiant energy appears like a continuum at macroscopic scale of intensity Granularity of light (in terms of photon) becomes manifest when magnified

19 19 The way how photon carries energy is in in contrast to the way wave carries energy. For wave the radiant energy is continuously distributed over a region in space and not in separate bundles (always recall the analogy of water in a hose and a stream of ping pong ball to help visualisation)

20 20 A beam of light if pictured as monochromatic wave (, ) A Energy flux of the beam is (in unit of joule per unit time per unit area) A beam of light pictured in terms of photons A Energy flux of the beam is S = n(hv)/At = n 0 c h  (in unit of joule per unit time per unit area). n is obtained by ‘counting’ the total number of photons in the beam volume, n = n 0 V = n 0 x (A ct), where n 0 is the photon number density of the radiation (in unit of number per unit volume) L = ct  h

21 21 Einstein’s Assumptions 1. The energy of a single photon is E = h. h is a proportional constant, called the Planck constant, that is to be determined experimentally With this assumption, a photon will have a momentum given by p = E/c = h/. This relation is obtained from SR relationship E 2 = p 2 c 2 + (m 0 c 2 ) 2, for which the mass of a photon is zero. Note that in classical physics momentum is intrinsically a particle attribute not defined for wave. By picturing light as particle (photon), the definition of momentum for radiation now becomes feasible


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