Mass of one electron = 9.109 x 10^-31 kg. Number weighing 1 g = 10^-3/(9.109 x 10^-31) = 1.10 x 10^27. One mole of electrons has mass = (6.022 x 10^23)(9.109 x 10^-31 kg) = 5.49 x 10^-7 kg = 5.49 x 10^-4 g. Charge = (6.022 x 10^23)(-1.602 x 10^-19 C) = -9.65 x 10^4 C.
(i) 1.10 x 10^27 electrons. (ii) Mass = 5.49 x 10^-4 g; charge = -9.65 x 10^4 C.
CH4 has 10 electrons per molecule, so 1 mol CH4 has 10NA = 6.022 x 10^24 electrons. In 7 mg of 14C, moles of carbon atoms = 0.007/14 = 5.0 x 10^-4 mol. Each 14C atom has 8 neutrons, so moles of neutrons = 0.004 mol and number = 0.004NA = 2.41 x 10^21. Their mass is (2.41 x 10^21)(1.675 x 10^-27) = 4.03 x 10^-6 kg. In 34 mg NH3, moles NH3 = 0.034/17 = 0.002 mol. Each molecule has 10 protons, so moles of protons = 0.020 mol and number = 1.20 x 10^22. Their mass is about (1.20 x 10^22)(1.673 x 10^-27) = 2.01 x 10^-5 kg. Changing temperature or pressure does not change the number of molecules in a given amount.
(i) 6.022 x 10^24 electrons. (ii) 2.41 x 10^21 neutrons; 4.03 x 10^-6 kg. (iii) 1.20 x 10^22 protons; 2.01 x 10^-5 kg. No, it depends on amount of NH3, not on temperature or pressure.
The complete nuclear symbol is written with mass number A and atomic number Z. Z = 17 is chlorine, Z = 92 is uranium and Z = 4 is beryllium. Therefore the symbols are ^35_17Cl, ^233_92U and ^9_4Be.
(i) 35Cl. (ii) 233U. (iii) 9Be.
lambda = 580 nm = 5.80 x 10^-7 m. Frequency nu = c/lambda = (3.00 x 10^8)/(5.80 x 10^-7) = 5.17 x 10^14 s^-1. Wave number = 1/lambda = 1.72 x 10^6 m^-1 = 1.72 x 10^4 cm^-1.
Frequency = 5.17 x 10^14 s^-1; wave number = 1.72 x 10^6 m^-1, or 1.72 x 10^4 cm^-1.
Use E = hnu = hc/lambda. (i) E = (6.626 x 10^-34)(3.0 x 10^15) = 1.99 x 10^-18 J. (ii) 0.50 A = 0.50 x 10^-10 m, so E = (6.626 x 10^-34)(3.0 x 10^8)/(0.50 x 10^-10) = 3.98 x 10^-15 J.
(i) 1.99 x 10^-18 J. (ii) 3.98 x 10^-15 J.
Frequency nu = 1/T = 1/(2.0 x 10^-10) = 5.0 x 10^9 s^-1. Wavelength lambda = c/nu = (3.0 x 10^8)/(5.0 x 10^9) = 6.0 x 10^-2 m. Wave number = 1/lambda = 16.7 m^-1.
Frequency = 5.0 x 10^9 s^-1; wavelength = 6.0 x 10^-2 m; wave number = 16.7 m^-1.
lambda = 4000 pm = 4.000 x 10^-9 m. Energy of one photon = hc/lambda = (6.626 x 10^-34)(3.0 x 10^8)/(4.000 x 10^-9) = 4.97 x 10^-17 J. Number of photons = 1/(4.97 x 10^-17) = 2.01 x 10^16.
2.01 x 10^16 photons.
Photon energy in eV = 1240/lambda(nm). Here lambda = 400 nm, so E = 1240/400 = 3.10 eV. Kinetic energy = 3.10 - 2.13 = 0.97 eV = 1.55 x 10^-19 J. From KE = (1/2)mv^2, v = sqrt(2KE/m_e) = sqrt[2(1.55 x 10^-19)/(9.109 x 10^-31)] = 5.84 x 10^5 m s^-1.
(i) 3.10 eV. (ii) 0.97 eV. (iii) 5.84 x 10^5 m s^-1.
Energy per photon = hc/lambda = (6.626 x 10^-34)(3.0 x 10^8)/(242 x 10^-9) = 8.21 x 10^-19 J. Per mole, energy = 8.21 x 10^-19 x 6.022 x 10^23 = 4.95 x 10^5 J mol^-1 = 495 kJ mol^-1.
4.95 x 10^2 kJ mol^-1.
lambda = 0.57 um = 5.7 x 10^-7 m. Energy per photon = hc/lambda = 3.49 x 10^-19 J. A 25 W source emits 25 J s^-1, so number of photons per second = 25/(3.49 x 10^-19) = 7.17 x 10^19.
7.17 x 10^19 photons s^-1.
At threshold, kinetic energy is zero, so nu0 = c/lambda. lambda = 6800 A = 6.800 x 10^-7 m. Hence nu0 = (3.0 x 10^8)/(6.800 x 10^-7) = 4.41 x 10^14 s^-1. Work function W0 = hnu0 = (6.626 x 10^-34)(4.41 x 10^14) = 2.92 x 10^-19 J = 1.82 eV.
Threshold frequency = 4.41 x 10^14 s^-1; work function = 2.92 x 10^-19 J, or 1.82 eV.
For hydrogen, 1/lambda = R(1/n1^2 - 1/n2^2) = R(1/2^2 - 1/4^2) = R(3/16). With R = 1.097 x 10^7 m^-1, 1/lambda = 2.06 x 10^6 m^-1, so lambda = 4.86 x 10^-7 m = 486 nm.
486 nm.
For hydrogen, ionisation energy from level n is 13.6/n^2 eV. For n = 5, E = 13.6/25 = 0.544 eV = 8.72 x 10^-20 J. From n = 1 the ionisation energy is 13.6 eV, so the n = 5 value is 1/25 as large.
0.544 eV per atom, or 8.72 x 10^-20 J per atom. This is 1/25 of the ground-state ionisation energy.
The maximum number of lines produced from level n is n(n - 1)/2. For n = 6, number of lines = 6 x 5/2 = 15.
15 emission lines.
For hydrogen, En = E1/n^2. Thus E5 = (-2.18 x 10^-18)/25 = -8.72 x 10^-20 J atom^-1. Radius rn = n^2a0, where a0 = 0.529 A. Therefore r5 = 25(0.529 A) = 13.2 A = 1.32 x 10^-9 m.
(i) -8.72 x 10^-20 J atom^-1. (ii) 1.32 x 10^-9 m, or 13.2 A.
The longest wavelength in the Balmer series corresponds to the smallest energy transition ending at n = 2, i.e. n = 3 to n = 2. Thus wave number = R(1/2^2 - 1/3^2) = R(5/36) = (1.097 x 10^7)(5/36) = 1.52 x 10^6 m^-1.
1.52 x 10^6 m^-1, or 1.52 x 10^4 cm^-1.
The given ground-state energy is -2.18 x 10^-11 erg = -2.18 x 10^-18 J. E5 = E1/25 = -8.72 x 10^-20 J. Energy required = E5 - E1 = 2.09 x 10^-18 J. If the electron returns from n = 5 to n = 1, the same energy is emitted as a photon. lambda = hc/E = (6.626 x 10^-34)(3.0 x 10^8)/(2.09 x 10^-18) = 9.50 x 10^-8 m = 95.0 nm.
Energy absorbed = 2.09 x 10^-18 J; wavelength emitted = 95.0 nm.
For n = 2, E2 = -2.18 x 10^-18/4 = -5.45 x 10^-19 J. To remove the electron to n = infinity, the required energy is 5.45 x 10^-19 J. The longest wavelength has exactly this energy: lambda = hc/E = (6.626 x 10^-34)(3.0 x 10^8)/(5.45 x 10^-19) = 3.65 x 10^-7 m = 3.65 x 10^-5 cm.
Energy required = 5.45 x 10^-19 J; longest wavelength = 3.65 x 10^-5 cm.
Use de Broglie's equation lambda = h/mv. With h = 6.626 x 10^-34 J s, m_e = 9.109 x 10^-31 kg and v = 2.05 x 10^7 m s^-1, lambda = 6.626 x 10^-34/[(9.109 x 10^-31)(2.05 x 10^7)] = 3.55 x 10^-11 m.
3.55 x 10^-11 m.
Momentum p = sqrt(2mK) = sqrt[2(9.1 x 10^-31)(3.0 x 10^-25)] = 7.39 x 10^-28 kg m s^-1. Hence lambda = h/p = (6.626 x 10^-34)/(7.39 x 10^-28) = 8.96 x 10^-7 m.
8.96 x 10^-7 m.
Count electrons by adding electrons for negative charge and subtracting for positive charge. Sodium ion has 10 electrons and magnesium ion has 10 electrons. Potassium ion, calcium ion, sulphide ion and argon each have 18 electrons.
Na+ and Mg2+ are isoelectronic with 10 electrons. K+, Ca2+, S2- and Ar are isoelectronic with 18 electrons.
H- has 2 electrons. Na+, O2- and F- each have 10 electrons, so their configuration is the neon configuration. For outermost electrons, 3s1 corresponds to Na (Z = 11), 2p3 to N (Z = 7), and 3p5 to Cl (Z = 17). The given noble-gas configurations identify Li, P and Sc respectively.
(i) H-: 1s2; Na+: 1s2 2s2 2p6; O2-: 1s2 2s2 2p6; F-: 1s2 2s2 2p6. (ii) 11, 7, 17. (iii) Li, P, Sc.
For a shell with principal quantum number n, allowed l values are 0 to n - 1. A g orbital has l = 4. Therefore the lowest n for which l = 4 is possible is n = 5.
n = 5.
For a 3d orbital, the principal quantum number is n = 3 and d means l = 2. The magnetic quantum number can have all integral values from -l to +l, so ml = -2, -1, 0, +1, +2.
n = 3, l = 2, and ml = -2, -1, 0, +1 or +2.
A neutral H2 molecule has 2 electrons. Adding one negative charge gives H2- with 3 electrons. A neutral O2 molecule has 16 electrons, and O2+ has lost one electron, so it has 15 electrons.
H2- has 3 electrons, H2 has 2 electrons and O2+ has 15 electrons.
For a given n, l can have values from 0 to n - 1. For each l, ml ranges from -l to +l. Thus for n = 3 the allowed l values are 0, 1 and 2. A d orbital has l = 2. The orbital 1p is impossible because n = 1 allows only l = 0; 3f is impossible because f means l = 3, but n = 3 allows only l = 0, 1, 2.
(i) l = 0, 1, 2; for l = 0, ml = 0; for l = 1, ml = -1, 0, +1; for l = 2, ml = -2, -1, 0, +1, +2. (ii) For 3d, l = 2 and ml = -2, -1, 0, +1, +2. (iii) 2s and 2p are possible; 1p and 3f are not possible.
The letter notation is l = 0 -> s, l = 1 -> p, l = 2 -> d, l = 3 -> f. Combine this with the given n value to name the orbital.
(a) 1s. (b) 3p. (c) 4d. (d) 4f.
n must be a positive integer, so n = 0 in (a) is impossible. For a given n, l can range only from 0 to n - 1; hence for n = 1, l = 1 in (c) is impossible, and for n = 3, l = 3 in (e) is impossible. In (b), (d) and (f), l is allowed, ml lies between -l and +l, and ms is +/-1/2.
Not possible: (a), (c) and (e). Possible: (b), (d) and (f).
For n = 4, the shell can hold 2n^2 = 32 electrons. Half can have ms = -1/2, so 16 electrons may have n = 4 and ms = -1/2. For n = 3, l = 0 is the 3s subshell, which has one orbital and can hold 2 electrons.
(a) 16 electrons. (b) 2 electrons.
Bohr's quantisation condition is mvr = nh/2π. Multiplying by 2π gives 2πr = nh/(mv). From de Broglie's relation, λ = h/(mv). Therefore 2πr = nλ. Thus the circumference of an allowed Bohr orbit contains an integral number n of electron wavelengths.
The circumference is 2πr = nλ, so it is an integral multiple of the de Broglie wavelength.
For a hydrogen-like ion, wave number is proportional to Z^2(1/n1^2 - 1/n2^2). For He+, Z = 2 and the 4 -> 2 transition gives 4R(1/2^2 - 1/4^2) = 4R(3/16) = 3R/4. In hydrogen, R(1/1^2 - 1/2^2) = 3R/4, so the same wavelength corresponds to transition n = 2 to n = 1.
The n = 2 to n = 1 transition in hydrogen.
For hydrogen-like species, ionisation energy from the ground state is Z^2 times the hydrogen value. For He+, Z = 2. Therefore energy required = 2^2(2.18 x 10^-18) = 8.72 x 10^-18 J atom^-1.
8.72 x 10^-18 J atom^-1.
Diameter of one carbon atom = 0.15 nm = 1.5 x 10^-10 m. Length = 20 cm = 0.20 m. Number of atoms = 0.20/(1.5 x 10^-10) = 1.33 x 10^9.
1.33 x 10^9 carbon atoms.
Diameter of one atom = total length/number of atoms = 2.4 cm/(2 x 10^8) = 1.2 x 10^-8 cm = 1.2 x 10^-10 m. Radius = half of diameter = 6.0 x 10^-11 m = 60 pm.
6.0 x 10^-11 m, or 60 pm.
Diameter = 2.6 A, so radius = 1.3 A = 130 pm. Also 2.6 A = 2.6 x 10^-8 cm. Number of atoms in 1.6 cm = 1.6/(2.6 x 10^-8) = 6.15 x 10^7.
(a) 130 pm. (b) 6.15 x 10^7 atoms.
Number of electrons = total charge/magnitude of electronic charge = (2.5 x 10^-16)/(1.602 x 10^-19) = 1.56 x 10^3.
1.56 x 10^3 electrons, approximately 1560 electrons.
Number of electrons = |q|/e = (1.282 x 10^-18)/(1.602 x 10^-19) = 8.00.
8 electrons.
Heavy nuclei such as gold have large positive charge and large mass, so alpha-particles experience strong repulsion and the target nucleus recoils little. A light aluminium nucleus has smaller nuclear charge and is less massive, so the repulsion is weaker and recoil is more appreciable. Therefore fewer alpha-particles would be scattered through large angles or bounced back.
Large-angle deflections and back scattering would be much less frequent.
In nuclide notation A/Z X, A is mass number and Z is atomic number. For bromine, Z is fixed at 35. The isotope with mass number 79 is therefore written as ^79_35Br. Because the symbol Br already identifies Z = 35, ^79Br is also meaningful. The alternatives with 35 as mass number or 79 as atomic number are not acceptable.
Mass number is written as the upper left superscript and atomic number as the lower left subscript. Since bromine has Z = 35 and the isotope has A = 79, 79/35Br and 79Br are acceptable, but 35/79Br and 35Br place or imply the wrong mass number.
Let the number of protons be Z. Then neutrons = 1.317Z. Mass number A = Z + 1.317Z = 2.317Z = 81, so Z = 34.96 ≈ 35. The element with atomic number 35 is bromine. Hence the atomic symbol is ^81_35Br.
^81_35Br.
Let protons be Z. A singly negative ion has electrons = Z + 1. Neutrons = 1.111(Z + 1). Since A = Z + neutrons = 37, Z + 1.111(Z + 1) = 37. This gives Z ≈ 17, so the ion is chlorine with mass number 37 and charge -1: ^37_17Cl-.
^37_17Cl-.
Let protons be Z. A 3+ ion has electrons = Z - 3. Neutrons = 1.304(Z - 3). Since A = Z + neutrons = 56, Z + 1.304(Z - 3) = 56. Thus 2.304Z = 59.912 and Z ≈ 26. The element is iron, so the ion is ^56_26Fe3+.
^56_26Fe3+.
In the electromagnetic spectrum, radio waves have the lowest frequencies among these, followed by microwaves, visible light, X-rays and cosmic rays. Amber light is visible light, so it lies above microwaves and below X-rays.
FM radio < microwave oven < amber light < X-rays < cosmic rays.
lambda = 616 nm = 6.16 x 10^-7 m. Frequency nu = c/lambda = 3.0 x 10^8/(6.16 x 10^-7) = 4.87 x 10^14 s^-1. Distance in 30 s = ct = (3.0 x 10^8)(30) = 9.0 x 10^9 m. Energy per quantum = hnu = (6.626 x 10^-34)(4.87 x 10^14) = 3.23 x 10^-19 J. Number of quanta for 2 J = 2/(3.23 x 10^-19) = 6.19 x 10^18.
(a) 4.87 x 10^14 s^-1. (b) 9.0 x 10^9 m. (c) 3.23 x 10^-19 J. (d) 6.19 x 10^18 quanta.
Energy of one photon is E = hc/lambda = (6.626 x 10^-34)(3.0 x 10^8)/(600 x 10^-9) = 3.31 x 10^-19 J. Number of photons = total energy/energy per photon = (3.15 x 10^-18)/(3.31 x 10^-19) = 9.51.
About 9.51 photons, so approximately 10 photons.
Frequency is nu = c/lambda. For 589 nm, nu1 = 3.0 x 10^8/(589 x 10^-9) = 5.093 x 10^14 Hz. For 589.6 nm, nu2 = 3.0 x 10^8/(589.6 x 10^-9) = 5.088 x 10^14 Hz. Energy difference = h(nu1 - nu2) = (6.626 x 10^-34)(5.18 x 10^11) = 3.43 x 10^-22 J.
Frequencies are 5.09 x 10^14 Hz and 5.09 x 10^14 Hz, more precisely 5.093 x 10^14 Hz and 5.088 x 10^14 Hz. Energy difference = 3.43 x 10^-22 J.
At threshold, W0 = hc/lambda0 = hnu0. With W0 = 1.9 eV, lambda0 = 1240/1.9 = 653 nm and nu0 = W0/h = 4.59 x 10^14 s^-1. For 500 nm radiation, photon energy = 1240/500 = 2.48 eV. Kinetic energy = 2.48 - 1.90 = 0.58 eV = 9.3 x 10^-20 J. From KE = (1/2)mv^2, v = sqrt(2KE/m_e) = 4.5 x 10^5 m s^-1.
(a) 653 nm. (b) 4.59 x 10^14 s^-1. For 500 nm radiation, kinetic energy = 0.58 eV = 9.3 x 10^-20 J and velocity = 4.5 x 10^5 m s^-1.
Photon energy = hc/lambda = 1240/256.7 = 4.83 eV. The stopping potential gives maximum kinetic energy = 0.35 eV. Therefore work function = 4.83 - 0.35 = 4.48 eV = 7.18 x 10^-19 J.
4.48 eV, or 7.18 x 10^-19 J.
Photon energy = hc/lambda = (6.626 x 10^-34)(3.0 x 10^8)/(150 x 10^-12) = 1.325 x 10^-15 J. Kinetic energy of the ejected electron = (1/2)mv^2 = 0.5(9.109 x 10^-31)(1.5 x 10^7)^2 = 1.025 x 10^-16 J. Binding energy = photon energy - kinetic energy = 1.22 x 10^-15 J = 7.63 x 10^3 eV.
1.22 x 10^-15 J, or 7.63 keV.
The frequency for 1285 nm is nu = c/lambda = 3.0 x 10^8/(1285 x 10^-9) = 2.33 x 10^14 Hz. Therefore nu/(3.29 x 10^15) = 0.07096 = 1/9 - 1/n^2. Hence 1/n^2 = 0.11111 - 0.07096 = 0.04015, so n^2 ≈ 24.9 and n ≈ 5. A wavelength of 1285 nm is in the infrared region.
n = 5; the line lies in the infrared region.
For hydrogen, rn = n^2a0 with a0 = 52.9 pm. The initial radius 1.3225 nm = 1322.5 pm = 25a0, so ni = 5. The final radius 211.6 pm = 4a0, so nf = 2. Thus the transition is 5 -> 2. Wave number = R(1/2^2 - 1/5^2), giving lambda = 4.34 x 10^-7 m = 434 nm. Since the final level is n = 2, it belongs to the Balmer series and lies in the visible region.
434 nm; Balmer series; visible region.
Use lambda = h/mv. lambda = 6.626 x 10^-34/[(9.109 x 10^-31)(1.6 x 10^6)] = 4.55 x 10^-10 m.
4.55 x 10^-10 m.
From lambda = h/mv, v = h/(m lambda). For a neutron, m = 1.675 x 10^-27 kg and lambda = 800 pm = 8.00 x 10^-10 m. Hence v = 6.626 x 10^-34/[(1.675 x 10^-27)(8.00 x 10^-10)] = 4.94 x 10^2 m s^-1.
4.94 x 10^2 m s^-1.
lambda = h/mv = 6.626 x 10^-34/[(9.109 x 10^-31)(2.19 x 10^6)] = 3.32 x 10^-10 m.
3.32 x 10^-10 m.
For the hockey ball, lambda = h/mv = 6.626 x 10^-34/[(0.1)(4.37 x 10^5)] = 1.52 x 10^-38 m.
1.52 x 10^-38 m.
Use the (n + l) rule. Electron 5 is 3p, with n + l = 4. Electrons 2 and 4 are 3d, with n + l = 5 and the same subshell energy. Electrons 3 and 6 are 4p, with n + l = 5 but higher n than 3d, so they have higher energy than 3d and equal energy to each other. Electron 1 is 4d, with n + l = 6, so it is highest among these.
Increasing energy: 5 < 2 = 4 < 3 = 6 < 1.
Outer-shell electrons are shielded by inner-shell electrons and are farther from the nucleus. Therefore a 4p electron in bromine is shielded more strongly than 2p and 3p electrons and experiences the lowest effective nuclear charge.
An electron in the 4p orbital experiences the lowest effective nuclear charge.
An orbital closer to the nucleus or with greater penetration experiences larger effective nuclear charge. 2s is closer than 3s. For the same n, penetration decreases in the order s > p > d > f, so 4d experiences larger effective nuclear charge than 4f, and 3p experiences larger effective nuclear charge than 3d.
(i) 2s. (ii) 4d. (iii) 3p.
Al and Si have their unpaired electrons in the same 3p subshell, but silicon has one more proton in the nucleus than aluminium. The additional nuclear charge is not completely cancelled by shielding, so the 3p electrons in Si experience greater effective nuclear charge.
The 3p electrons in silicon experience more effective nuclear charge.
P is [Ne]3s2 3p3, so three 3p electrons are unpaired. Si is [Ne]3s2 3p2, so two are unpaired. Cr is [Ar]3d5 4s1, giving six unpaired electrons. Fe is [Ar]3d6 4s2, giving four unpaired 3d electrons. Kr has a closed-shell configuration, so it has no unpaired electron.
(a) P: 3. (b) Si: 2. (c) Cr: 6. (d) Fe: 4. (e) Kr: 0.
For n = 4, possible l values are 0, 1, 2 and 3, corresponding to 4s, 4p, 4d and 4f: four subshells. The n = 4 shell contains n^2 = 16 orbitals and 2n^2 = 32 electrons. One electron in each orbital can have ms = -1/2, so 16 electrons can have ms = -1/2.
(a) 4 subshells. (b) 16 electrons.