12.E: Quantum Mechanics (Exercise)

Conceptual Questions

12.2: Blackbody Radiation

Conceptual Questions

Exercise 1
Give an example of a physical entity that is quantized. State specifically what the entity is and what the limits are on its values.
Exercise 2
Give an example of a physical entity that is not quantized, in that it is continuous and may have a continuous range of values.
Exercise 3
What aspect of the blackbody spectrum forced Planck to propose quantization of energy levels in the thermal oscillators?
Exercise 4
Why don’t we notice quantization in everyday events?

12.3: The Photoelectric Effect

Conceptual Questions

Exercise 5
Is visible light the only type of EM radiation that can cause the photoelectric effect?
Exercise 6
Which aspects of the photoelectric effect cannot be explained without photons? Which can be explained without photons? Are the latter inconsistent with the existence of photons?
Exercise 7
Is the photoelectric effect a direct consequence of the wave character of EM radiation or of the particle character of EM radiation? Explain briefly.
Exercise 8
Insulators (nonmetals) have a higher BE than metals, and it is more difficult for photons to eject electrons from insulators. Discuss how this relates to the free charges in metals that make them good conductors.
Exercise 9
If you pick up and shake a piece of metal that has electrons in it free to move as a current, no electrons fall out. Yet if you heat the metal, electrons can be boiled off. Explain both of these facts as they relate to the amount and distribution of energy involved with shaking the object as compared with heating it.

12.4: The Wave Nature of Matter

Conceptual Questions

Exercise 10
How does the interference of water waves differ from the interference of electrons? How are they analogous?
Exercise 11
Describe one type of evidence for the wave nature of matter.
Exercise 12
Describe one type of evidence for the particle nature of EM radiation.

12.5: Uncertainty Principle

Conceptual Questions

Exercise 13
What is the Heisenberg uncertainty principle? Does it place limits on what can be known?

12.6: Discovery of the Atomic Nucleus

Conceptual Questions

Exercise 14
What two pieces of evidence allowed the first calculation of me, the mass of the electron?
(a) The ratios qe/me and qp/mp.
(b) The values of qe and EB.
(c) The ratio qe/me and qe.
Justify your response.
Exercise 15
How do the allowed orbits for electrons in atoms differ from the allowed orbits for planets around the sun? Explain how the correspondence principle applies here.

12.7: Bohr’s Theory of the Hydrogen Atom

Conceptual Questions

Exercise 16
How do the allowed orbits for electrons in atoms differ from the allowed orbits for planets around the sun? Explain how the correspondence principle applies here.
Exercise 17
Explain how Bohr’s rule for the quantization of electron orbital angular momentum differs from the actual rule.
Exercise 18
What is a hydrogen-like atom, and how are the energies and radii of its electron orbits related to those in hydrogen?

12.8: The Wave Nature of Matter Causes Quantization

Conceptual Questions

Exercise 19
How is the de Broglie wavelength of electrons related to the quantization of their orbits in atoms and molecules?

Problems & Exercises

12.2: Blackbody Radiation

Problems & Exercises

Exercise 20
A LiBr molecule oscillates with a frequency of 1.7×1013 Hz. (a) What is the difference in energy in eV between allowed oscillator states? (b) What is the approximate value of n for a state having an energy of 1.0 eV?
Solution
(a) 0.070 eV
(b) 14
Exercise 21
The difference in energy between allowed oscillator states in HBr molecules is 0.330 eV. What is the oscillation frequency of this molecule?
Exercise 22
A physicist is watching a 15-kg orangutan at a zoo swing lazily in a tire at the end of a rope. He (the physicist) notices that each oscillation takes 3.00 s and hypothesizes that the energy is quantized. (a) What is the difference in energy in joules between allowed oscillator states? (b) What is the value of n for a state where the energy is 5.00 J? (c) Can the quantization be observed?

12.3: The Photoelectric Effect

Problems & Exercises

Exercise 23
What is the longest-wavelength EM radiation that can eject a photoelectron from silver, given that the binding energy is 4.73 eV? Is this in the visible range?
Solution
263 nm
Exercise 24
Find the longest-wavelength photon that can eject an electron from potassium, given that the binding energy is 2.24 eV. Is this visible EM radiation?
Exercise 25
What is the binding energy in eV of electrons in magnesium, if the longest-wavelength photon that can eject electrons is 337 nm?
Solution
3.69 eV
Exercise 26
Calculate the binding energy in eV of electrons in aluminum, if the longest-wavelength photon that can eject them is 304 nm.
Exercise 27
What is the maximum kinetic energy in eV of electrons ejected from sodium metal by 450-nm EM radiation, given that the binding energy is 2.28 eV?
Solution
0.483 eV
Exercise 28
UV radiation having a wavelength of 120 nm falls on gold metal, to which electrons are bound by 4.82 eV. What is the maximum kinetic energy of the ejected photoelectrons?
Exercise 29
Violet light of wavelength 400 nm ejects electrons with a maximum kinetic energy of 0.860 eV from sodium metal. What is the binding energy of electrons to sodium metal?
Solution
2.25 eV
Exercise 30
UV radiation having a 300-nm wavelength falls on uranium metal, ejecting 0.500-eV electrons. What is the binding energy of electrons to uranium metal?
Exercise 31
What is the wavelength of EM radiation that ejects 2.00-eV electrons from calcium metal, given that the binding energy is 2.71 eV? What type of EM radiation is this?
Solution
(a) 264 nm
(b) Ultraviolet
Exercise 32
Find the wavelength of photons that eject 0.100-eV electrons from potassium, given that the binding energy is 2.24 eV. Are these photons visible?
Exercise 33
A laser with a power output of 2.00 mW at a wavelength of 400 nm is projected onto calcium metal. (a) How many electrons per second are ejected? (b) What power is carried away by the electrons, given that the binding energy is 2.71 eV?
Solution
(a) 4.02×1015/s
(b) 0.256 mW
Exercise 34
(a) Calculate the number of photoelectrons per second ejected from a 1.00-mm 2 area of sodium metal by 500-nm EM radiation having an intensity of 1.30 kW/m2 (the intensity of sunlight above the Earth’s atmosphere). (b) Given that the binding energy is 2.28 eV, what power is carried away by the electrons? (c) The electrons carry away less power than brought in by the photons. Where does the other power go? How can it be recovered?
Exercise 35
Unreasonable Results
Red light having a wavelength of 700 nm is projected onto magnesium metal to which electrons are bound by 3.68 eV. (a) Use KE e=hfBE to calculate the kinetic energy of the ejected electrons. (b) What is unreasonable about this result? (c) Which assumptions are unreasonable or inconsistent?
Solution
(a) –1.90 eV
(b) Negative kinetic energy
(c) That the electrons would be knocked free.
Exercise 36
Unreasonable Results
(a) What is the binding energy of electrons to a material from which 4.00-eV electrons are ejected by 400-nm EM radiation? (b) What is unreasonable about this result? (c) Which assumptions are unreasonable or inconsistent?

12.4: The Wave Nature of Matter

Problems & Exercises

Exercise 37
At what velocity will an electron have a wavelength of 1.00 m?
Solution
7.28×10–4 m
Exercise 38
What is the wavelength of an electron moving at 3.00% of the speed of light?
Exercise 39
At what velocity does a proton have a 6.00-fm wavelength (about the size of a nucleus)? Assume the proton is nonrelativistic. (1 femtometer = 1015m.)
Solution
6.62×107 m/s
Exercise 40
What is the velocity of a 0.400-kg billiard ball if its wavelength is 7.50 cm (large enough for it to interfere with other billiard balls)?
Exercise 41
Find the wavelength of a proton moving at 1.00% of the speed of light.
Solution
1.32×10–13 m
Exercise 42
Experiments are performed with ultracold neutrons having velocities as small as 1.00 m/s. (a) What is the wavelength of such a neutron? (b) What is its kinetic energy in eV?
Exercise 43
(a) Find the velocity of a neutron that has a 6.00-fm wavelength (about the size of a nucleus). Assume the neutron is nonrelativistic. (b) What is the neutron’s kinetic energy in MeV?
Solution
(a) 6.62×107 m/s
(b) 22.9 MeV
Exercise 44
What is the wavelength of an electron accelerated through a 30.0-kV potential, as in a TV tube?
Exercise 45
What is the kinetic energy of an electron in a TEM having a 0.0100-nm wavelength?
Solution
15.1 keV
(12.E.1)
Exercise 46
(a) Calculate the velocity of an electron that has a wavelength of 1.00 μm. (b) Through what voltage must the electron be accelerated to have this velocity?
Exercise 47
The velocity of a proton emerging from a Van de Graaff accelerator is 25.0% of the speed of light. (a) What is the proton’s wavelength? (b) What is its kinetic energy, assuming it is nonrelativistic? (c) What was the equivalent voltage through which it was accelerated?
Solution
(a) 5.29 fm
(b) 4.70×1012 J
(c) 29.4 MV
Exercise 48
The kinetic energy of an electron accelerated in an X-ray tube is 100 keV. Assuming it is nonrelativistic, what is its wavelength?
Exercise 49
Unreasonable Results
(a) Assuming it is nonrelativistic, calculate the velocity of an electron with a 0.100-fm wavelength (small enough to detect details of a nucleus). (b) What is unreasonable about this result? (c) Which assumptions are unreasonable or inconsistent?
Solution
(a) 7.28×1012 m/s
(b) This is thousands of times the speed of light (an impossibility).
(c) The assumption that the electron is non-relativistic is unreasonable at this wavelength.

12.5: Uncertainty Principle

Problems & Exercises

Exercise 50
(a) If the position of an electron in a membrane is measured to an accuracy of 1.00 μm, what is the electron’s minimum uncertainty in velocity? (b) If the electron has this velocity, what is its kinetic energy in eV? (c) What are the implications of this energy, comparing it to typical molecular binding energies?
Solution
(a) 57.9 m/s
(b) 9.55×109 eV
(c) Typical molecular binding energies range from about 1eV to 10 eV, therefore the result in part (b) is approximately 9 orders of magnitude smaller than typical molecular binding energies.
Exercise 51
(a) If the position of a chlorine ion in a membrane is measured to an accuracy of 1.00 μm, what is its minimum uncertainty in velocity, given its mass is 5.86×1026 kg? (b) If the ion has this velocity, what is its kinetic energy in eV, and how does this compare with typical molecular binding energies?
Exercise 52
Suppose the velocity of an electron in an atom is known to an accuracy of 2.0×103 m/s (reasonably accurate compared with orbital velocities). What is the electron’s minimum uncertainty in position, and how does this compare with the approximate 0.1-nm size of the atom?
Solution
29 nm,
290 times greater
Exercise 53
The velocity of a proton in an accelerator is known to an accuracy of 0.250% of the speed of light. (This could be small compared with its velocity.) What is the smallest possible uncertainty in its position?
Exercise 54
A relatively long-lived excited state of an atom has a lifetime of 3.00 ms. What is the minimum uncertainty in its energy?
Solution
1.10×1013 eV
Exercise 55
(a) The lifetime of a highly unstable nucleus is 1020 s. What is the smallest uncertainty in its decay energy? (b) Compare this with the rest energy of an electron.
Exercise 56
The decay energy of a short-lived particle has an uncertainty of 1.0 MeV due to its short lifetime. What is the smallest lifetime it can have?
Solution
3.3×1022 s
Exercise 57
The decay energy of a short-lived nuclear excited state has an uncertainty of 2.0 eV due to its short lifetime. What is the smallest lifetime it can have?
Exercise 58
What is the approximate uncertainty in the mass of a muon, as determined from its decay lifetime?
Solution
2.66×1046 kg
Exercise 59
Derive the approximate form of Heisenberg’s uncertainty principle for energy and time, ΔEΔth, using the following arguments: Since the position of a particle is uncertain by Δxλ, where λ is the wavelength of the photon used to examine it, there is an uncertainty in the time the photon takes to traverse Δx. Furthermore, the photon has an energy related to its wavelength, and it can transfer some or all of this energy to the object being examined. Thus the uncertainty in the energy of the object is also related to λ. Find Δt and ΔE; then multiply them to give the approximate uncertainty principle.

12.6: Discovery of the Atomic Nucleus

Problem Exercises

Exercise 60
Rutherford found the size of the nucleus to be about 1015 m. This implied a huge density. What would this density be for gold?
Solution
6×1020kg/m3
Exercise 61
In Millikan’s oil-drop experiment, one looks at a small oil drop held motionless between two plates. Take the voltage between the plates to be 2033 V, and the plate separation to be 2.00 cm. The oil drop (of density 0.81 g/cm3) has a diameter of 4.0×106 m. Find the charge on the drop, in terms of electron units.
Exercise 62
(a) An aspiring physicist wants to build a scale model of a hydrogen atom for her science fair project. If the atom is 1.00 m in diameter, how big should she try to make the nucleus?
(b) How easy will this be to do?
Solution
(a) 10.0 μm
(b) It isn’t hard to make one of approximately this size. It would be harder to make it exactly 10.0 μm.

12.7: Bohr’s Theory of the Hydrogen Atom

Problems & Exercises

Exercise 63
By calculating its wavelength, show that the first line in the Lyman series is UV radiation.
Solution
1λ=R(1nf21ni2)λ=1R[(ninf)2ni2nf2];ni=2,nf=1, so that
λ=(m1.097×107)[(2×1)22212]=1.22×107 m=122 nm , which is UV radiation.
Exercise 64
Find the wavelength of the third line in the Lyman series, and identify the type of EM radiation.
Exercise 65
Look up the values of the quantities in aB=h24π2mekqe2, and verify that the Bohr radius aB is 0.529×1010 m.
Solution
aB=h24π2mekZqe2=(6.626×1034 J·s)24π2(9.109×1031 kg)(8.988×109 N· m2/C2)(1)(1.602×1019 C)2=0.529×1010 m
Exercise 66
Verify that the ground state energy E0 is 13.6 eV by using E0=2π2qe4mek2h2.
Exercise 67
If a hydrogen atom has its electron in the n=4 state, how much energy in eV is needed to ionize it?
Solution
0.850 eV
Exercise 68
A hydrogen atom in an excited state can be ionized with less energy than when it is in its ground state. What is n for a hydrogen atom if 0.850 eV of energy can ionize it?
Exercise 69
Find the radius of a hydrogen atom in the n=2 state according to Bohr’s theory.
Solution
2.12×10–10 m
Exercise 70
Show that (13.6 eV)/hc=1.097×107 m=R (Rydberg’s constant), as discussed in the text.
Exercise 71
What is the smallest-wavelength line in the Balmer series? Is it in the visible part of the spectrum?
Solution
365 nm
It is in the ultraviolet.
Exercise 72
Show that the entire Paschen series is in the infrared part of the spectrum. To do this, you only need to calculate the shortest wavelength in the series.
Exercise 73
Do the Balmer and Lyman series overlap? To answer this, calculate the shortest-wavelength Balmer line and the longest-wavelength Lyman line.
Solution
No overlap
365 nm
122 nm
Exercise 74
(a) Which line in the Balmer series is the first one in the UV part of the spectrum?
(b) How many Balmer series lines are in the visible part of the spectrum?
(c) How many are in the UV?
Exercise 75
A wavelength of 4.653 μm is observed in a hydrogen spectrum for a transition that ends in the nf=5 level. What was ni for the initial level of the electron?
Solution
7
Exercise 76
A singly ionized helium ion has only one electron and is denoted He+. What is the ion’s radius in the ground state compared to the Bohr radius of hydrogen atom?
Exercise 77
A beryllium ion with a single electron (denoted Be3+) is in an excited state with radius the same as that of the ground state of hydrogen.
(a) What is n for the Be3+ ion?
(b) How much energy in eV is needed to ionize the ion from this excited state?
Solution
(a) 2
(b) 54.4 eV
Exercise 78
Atoms can be ionized by thermal collisions, such as at the high temperatures found in the solar corona. One such ion is C+5, a carbon atom with only a single electron.
(a) By what factor are the energies of its hydrogen-like levels greater than those of hydrogen?
(b) What is the wavelength of the first line in this ion’s Paschen series?
(c) What type of EM radiation is this?
Exercise 79
Verify Equations rn=n2ZaB and aB=h24π2mekqe2=0.529×1010 m using the approach stated in the text. That is, equate the Coulomb and centripetal forces and then insert an expression for velocity from the condition for angular momentum quantization.
Solution
kZqe2rn2=meV2rn , so that rn=kZqe2meV2=kZqe2me1V2. From the equation mevrn=nh2π , we can substitute for the velocity, giving: rn=kZqe2me4π2me2rn2n2h2 so that rn=n2Zh24π2mekqe2=n2ZaB , where aB=h22mekqe2.
Exercise 80
The wavelength of the four Balmer series lines for hydrogen are found to be 410.3, 434.2, 486.3, and 656.5 nm. What average percentage difference is found between these wavelength numbers and those predicted by 1λ=R(1nf21ni2)? It is amazing how well a simple formula (disconnected originally from theory) could duplicate this phenomenon.