1 PHYS-271 HOMEWORK #1 Due on Wednesday Feb 1st at 9h25 in class. Late homework will not be graded. 1. On the Planck Constant and Planck Scales Planck realized the great importance of his constant h beyond a simple fitting parameter in the quantum theory of light. In fact, he proposed that using the fundamental constant h, c (the speed of light) and G (Newton’s gravitational constant) one can construct a natural set of units, or scales, related to length, time and mass. Discuss the scales that you found here in relation to other scales that you know. 1 1 1 2 a) Show that the expressions ( hG ) 2 , ( hG ) 2 , and ( hc G ) have dimensions of length, time c3 c5 and mass and compute their numerical values. These quantities are known as Planck length, Planck time, and Planck mass. b) Assume now that h is much larger, and given by h = 1 J · s. Re-calculate the Planck length, time and mass. What do you tentatively conclude? 2. Light Quantization and the Photoelectric Effect a) Calculate the energy of a photon whose frequency is a) 5 x 1014 Hz, b) 10 GHz and c) 30 MHz. Express your answer in electron volts. b) Determine the corresponding wavelengths for the photons given in a). c) An FM radio transmitter has a power output of 100 kW and operates at 94 MHz. How many photons per second does the transmitter emit? d) The average power generated by the Sun is 3.74 x 1026 W. Assuming the average wavelength is 500 nm, find the number of photons emitted in 1 s. e) The photocurrent of a photocell is cut off by a retarding potential of 2.92 V for radiation at 250 nm. Find the work function for the material. f) Light of wavelength 500 nm is incident on a metallic surface. If the stopping potential for the photoelectric effect is 0.45V, find i) the maximum energy of the emitted electrons, ii) the work function and iii) the cutoff wavelength. g) A light source of wavelength λ illuminates a metal and ejects photoelectrons with a maximum kinetic energy of 1.00 eV. A second light source with half the wavelength of the first 2 ejects photoelectrons with a maximum kinetic energy of 4.00 eV. What is the work function for the metal? 3. The de Broglie Waves of Matter a) Calculate the de Broglie wavelength for a proton moving with a speed of 106 m/s. b) Calculate the de Broglie wavelength for an electron with kinetic energy i) 50 eV and ii) 50 keV. c) Calculate the de Broglie wavelength of a 74 kg person running at a speed of 5 m/s. Will this person “interfere” with a door 1 meter wide? d) Calculate what would h need to be for this person to “interfere” with the 1m wide door. e) Show that the de Broglie wavelength of an √ electron accelerated from rest through a small potential difference V is given by λ = 1.226/ V , where λ is in nanometers and V is in volts. f) An electron has a de Broglie wavelength equal to the diameter of the hydrogen atom. What is the kinetic energy of the electron? Compare it with the the ground state energy of the hydrogen atom, =13.6 eV. Phys 271:Assignment 1-Solutions 1. (a) [c] = LT −1 [h] = L2 M T −1 [G] = L3 M −1 T −2 `p = hG c3 1/2 −→ [`p ] = [h]1/2 [G]1/2 [c]−3/2 = (L2 M T −1 )1/2 (L3 M −1 T −2 )1/2 (LT −1 )−3/2 = L(1+3/2−3/2) M (1/2−1/2) T (−1/2−1+3/2) =L Similarly, one can verify [tp ] = T and [mp ] = M . Alternatively, let `p = cx hy Gz . Then [`p ] = L = [c]x [h]y [G]z = (LT −1 )x (L2 M T −1 )y (L3 M −1 T −2 )z = L(x+2y+3z) T (−x−y−2z) M (y−z) . =⇒ x + 2y + 3z = 1 x + y + 2z = 0 y−z =0 ∴ x = −3/2, y = 1/2, z = 1/2. So `p = hG c3 1/2 . /2 Numerical values are: `p = 4.0501 × 10−35 m tp = 1.3510 × 10−43 s mp = 5.4573 × 10−8 kg /1.5 (b) Assume that h = 1 J s . Then `p = 1.5734 × 10−18 m tp = 5.2483 × 10−27 s mp = 2.1201 × 109 kg . /1.5 1 2. (a) i. E1 = hν1 = 2.0678 eV ii. E2 = hν2 = 4.1357 × 10−5 eV iii. E3 = hν3 = 1.2407 × 10−7 eV /1.5 (b) i. λ1 = c = 5.9958 × 10−7 m ν1 ii. λ2 = 2.9979 × 10−2 m iii. λ3 = 9.9931 m /1 (c) n= Etotal Pt = = 1.6055 × 1030 Ephoton hν /1 (d) n= Pt Ephoton = P tλ = 9.4138 × 1044 hc /1 (e) Ephoton = hc = 4.9594 eV λ ϕ = Ephoton − Kelectron = 2.0394 eV /2 (f) Ephoton = hc = 2.4797 eV λ 2 i. Kmax = 0.45 eV ii. ϕ = Ephoton − Kmax = 2.0297 eV iii. λcutof f = hc = 6.1085 × 10−7 m ϕ /1.5 (g) (1) hc λ hc (1) = = 2Ephoton λ/2 Ephoton = (2) Ephoton (1) (1) Kmax = Ephoton − ϕ (2) (1) (2) Kmax = Ephoton − ϕ = 2Ephoton − ϕ (2) (1) =⇒ Kmax − Kmax =ϕ ϕ = 2.00 eV /2 3. (a) h = 3.9615 × 10−13 m . mv λ= /1 (b) p2 2m √ =⇒ p = 2mK K= i. For K = 50 eV, λ= √ h = 1.7346 × 10−10 m . 2mK ii. For K = 50 keV, λ = 5.4854 × 10−12 m 3 /3 (c) λ= h = 1.7908 × 10−36 m mv λ << 1 m ∴ the person will not interfere with the door. /1 (d) In order for the person to ‘interfere’ with the door the de Broglie wavelength must be approximately of the order of the width of the door, in analogy with light passing through a single slit. So h ∼1m mv =⇒ h ∼ (1 m )mv = 370 J s ∴ h ∼ 100 J s . /1 (e) K = eV −→ K = |V | in eV So −→ p2 K=V = 2m √ p = 2mV So λ= h h hc 1 √ =√ =√ 2 p 2mV 2mc V (1240 eV nm ) 1 √ =p 2(5.11 × 105 eV ) V 1 ≈ 1.266 √ nm V /2 (f) Take the radius of the hydrogen atom to be the Bohr radius. h = 2a0 p h p= 2a0 λ= Then K= p2 h2 = = 134 eV 2m 8ma20 /2 4
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