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1 The Quantum Mechanical Model of the Atom Chapter 7
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2 The nature of light Light is electromagnetic radiation: a wave of oscillating electric & magnetic fields.
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3 Wave properties A wave has wavelength, frequency, and amplitude
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4 Wave properties Wavelength = (lambda), in m Frequency = (nu), in cycles/sec or s -1 Wavelength & frequency related by wave speed: Speed of light c = 3.00 x 10 8 m s -1
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5 Example1 Calculate the frequency of light with = 589 nm
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6 Example 1 Calculate the frequency of light with = 589 nm = cc = 3.00 x 10 8 m s -1 Must convert nm to m so units agree (n = 10 -9 )
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7 Example 2 Calculate the wavelength in nm of light with = 9.83 x 10 14 s -1
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8 Electromagnetic spectrum = all wavelengths of electromagnetic radiation
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9 Photoelectric effect Light shining on metal surface can cause metal to emit e - (measured as electric current)
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10 Photoelectric effect Classical theory more e - emitted if light either brighter (amplitude) or more energetic (shorter ) e – still emitted in dim light if given enough time for e - to gather enough energy to escape
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11 Photoelectric effect Observations do not match classical predictions! A threshold frequency exists for e - emission: no e - emitted below that regardless of brightness Above threshold, e - emitted even with dim light No lag time for e - emission in high, dim light
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12 Albert Einstein explains photoelectric effect Light comes in packets or particles called photons Amount of energy in a photon related to its frequency h = 6.626 x 10 -34 J s
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13 Example 3 What is the energy of a photon with wavelength 242.4 nm?
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14 Example 4 A Cl 2 molecule has bond energy = 243 kJ/mol. Calculate the minimum photon frequency required to dissociate a Cl 2 molecule.
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15 Example 4
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16 Example 4 What color is this photon? A photon with wavelength 492 nm is blue
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17 Example 4 A Cl 2 molecule has bond energy = 243 kJ/mol. Calculate minimum photon frequency to dissociate a Cl 2 molecule. What color is this photon? A photon with wavelength 492 nm is blue
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18 Emission spectra When atom absorbs energy it may re-emit the energy as light
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19 Emission spectra White light spectrum is continuous Atomic emission spectrum is discontinuous Each substance has a unique line pattern
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20 Hydrogen emission spectrum Visible lines at 410 nm (far violet) 434 nm (violet) 486 nm (blue-green) 656 nm (red)
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21 Emission spectra Classical theories could not explain Why atomic emission spectra were not continuous Why electron doesn’t continuously emit energy as it spirals into the nucleus
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22 Bohr model Niels Bohr’s model to explain atomic spectra electron = particle in circular orbit around nucleus Only certain orbits (called stationary states) can exist r n = orbit radius, n = positive integer, a 0 = 53 pm Electron in stationary state has constant energy R H = 2.179 x 10 –18 J Bohr model is quantized
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23 Bohr model e – can pass only from one allowed orbit to another When making a transition, a fixed quantum of energy is involved
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25 Bohr model Bohr model Calculate the wavelength of light emitted when the hydrogen electron jumps from n=4 to n=2 Photon energy is an absolute amount of energy Electron absorbs photon, ∆E electron is + Electron emits photon, ∆E electron is –
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26 Bohr model Bohr model Calculate the wavelength of light emitted when the hydrogen electron jumps from n=4 to n=2 486 nm corresponds to the blue-green line
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27 Example Example What wavelength of light will cause the H electron to jump from n=1 to n=3? To what region of the electromagnetic spectrum does this photon belong?
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28 Example Example What wavelength of light will cause the H electron to pass from n=1 to n=3?
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29 Example Example What wavelength of light will cause the H electron to pass from n=1 to n=3? The atom must absorb an ultraviolet photon with = 103 nm
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30 Light has both particle & wave behaviors Wave nature shown by diffraction
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31 Light has both particle & wave behaviors Particle nature shown by photoelectric effect
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32 Electrons also have wave properties Individual electrons exhibit diffraction, like waves How can e – be both particle & wave?
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33 Complementarity Without laser, single e – produces diffraction pattern (wave-like) With laser, single e – makes a flash behind one slit or the other, indicating which slit it went through – – and diffraction pattern is gone (particle-like) We can never simultaneously see the interference pattern and know which slit the e – goes through
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34 Complementarity Complementary properties exclude each other If you know which slit the e – passes through (particle), you lose the diffraction pattern (wave) If you see interference (wave), you lose information about which slit the e – passes through (particle) Heisenberg uncertainty principle sets limit on what we can know
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35 Indeterminancy Classical outcome is predictable from starting conditions Quantum-mechanical outcome not predictable but we can describe probability region
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36 Electrons & probability Schrodinger applied wave mechanics to electrons Equation (wave function, ) describe e – energy Equation requires 3 integers (quantum numbers) Plot of 2 gives a probability distribution map of e – location = orbital Schrodinger wave functions successfully predict energies and spectra for all atoms
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37 Quantum numbers Principal quantum number, n Determines size and overall energy of orbital Positive integer 1, 2, 3... Corresponds to Bohr energy levels
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38 Quantum numbers Angular momentum quantum number, l Determines shape of orbital Positive integer 0, 1, 2... (n–1) Corresponds to sublevels l letter 0s 1p 2d 3f
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39 Quantum numbers Magnetic quantum number, m l Determines number of orbitals in a sublevel and orientation of each orbital in xyz space integers –l... 0... +l
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41 Shapes of orbitals s orbital (l = 0, m l = 0) p orbitals (l = 1, m l = –1, 0, +1)
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42 Shapes of orbitals d orbitals (l = 2, m l = –2, –1, 0, +1, +2)
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43 What type of orbital is designated by each set of quantum numbers? n = 5, l = 1, m l = 0 n = 4, l = 2, m l = –2 n = 2, l = 0, m l = 0 Write a set of quantum numbers for each orbital 4s 3d 5p
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44 What type of orbital is designated by each set of quantum numbers? n = 5, l = 1, m l = 05p n = 4, l = 2, m l = –24d n = 2, l = 0, m l = 02s Write a set of quantum numbers for each orbital 4s n = 4, l = 0, m l = 0 3d n = 3, l = 2, m l = –2, –1, 0, +1, or +2 5p n = 5, l = 1, m l = –1, 0, or +1
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46 Electron configurations Aufbau principle: e – takes lowest available energy Hund’s rule: if there are 2 or more orbitals of equal energy (degenerate orbitals), e – will occupy all orbitals singly before pairing Pauli principle: Adds a 4th quantum number, m s (spin) No two e – in an atom can have the same set of 4 quantum numbers ⇒ 2 e – per orbital
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