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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Chapter 7 The Quantum– Mechanical Model of the Atom Roy Kennedy Massachusetts Bay Community College Wellesley Hills, MA Chemistry: A Molecular Approach, 2nd Ed. Nivaldo Tro
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Beginnings of Quantum Mechanics Until the beginning of the 20 th century it was believed that all physical phenomena were deterministic Work done at that time by many famous physicists discovered that for sub-atomic particles, the present condition does not determine the future condition Albert Einstein, Neils Bohr, Louis de Broglie, Max Planck, Werner Heisenberg, P. A. M. Dirac, and Erwin Schrödinger Quantum mechanics forms the foundation of chemistry – explaining the periodic table and the behavior of the elements in chemical bonding – as well as providing the practical basis for lasers, computers, and countless other applications 2 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Behavior of the Very Small Electrons are incredibly small a single speck of dust has more electrons than the number of people who have ever lived on earth Electron behavior determines much of the behavior of atoms Directly observing electrons in the atom is impossible, the electron is so small that observing it changes its behavior even shining a light on the electron would affect it 3 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e A Theory that Explains Electron Behavior The quantum-mechanical model explains the manner in which electrons exist and behave in atoms It helps us understand and predict the properties of atoms that are directly related to the behavior of the electrons why some elements are metals and others are nonmetals why some elements gain one electron when forming an anion, whereas others gain two why some elements are very reactive while others are practically inert and other periodic patterns we see in the properties of the elements 4 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Nature of Light: Its Wave Nature Light is a form of electromagnetic radiation composed of perpendicular oscillating waves, one for the electric field and one for the magnetic field an electric field is a region where an electrically charged particle experiences a force a magnetic field is a region where a magnetized particle experiences a force All electromagnetic waves move through space at the same, constant speed 3.00 x 10 8 m/s in a vacuum = the speed of light, c 5 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Electromagnetic Radiation 6 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Speed of Energy Transmission 7 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Characterizing Waves The amplitude is the height of the wave the distance from node to crest or node to trough the amplitude is a measure of how intense the light is – the larger the amplitude, the brighter the light The wavelength ( ) is a measure of the distance covered by the wave the distance from one crest to the next or the distance from one trough to the next, or the distance between alternate nodes 8 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Wave Characteristics 9 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Characterizing Waves The frequency ( ) is the number of waves that pass a point in a given period of time the number of waves = number of cycles units are hertz (Hz) or cycles/s = s −1 1 Hz = 1 s −1 The total energy is proportional to the amplitude of the waves and the frequency the larger the amplitude, the more force it has the more frequently the waves strike, the more total force there is 10 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Relationship Between Wavelength and Frequency For waves traveling at the same speed, the shorter the wavelength, the more frequently they pass This means that the wavelength and frequency of electromagnetic waves are inversely proportional because the speed of light is constant, if we know wavelength we can find the frequency, and vice versa 11 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Example 7.1: Calculate the wavelength of red light with a frequency of 4.62 x 10 14 s −1 the unit is correct, the wavelength is appropriate for red light Check: Solve: ∙ = c, 1 nm = 10 −9 m Conceptual Plan: Relationships: = 4.62 x 10 14 s −1, (nm) Given: Find: (s −1 ) (m) (nm) 12 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Practice – Calculate the wavelength of a radio signal with a frequency of 100.7 MHz 13 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Practice – Calculate the wavelength of a radio signal with a frequency of 100.7 MHz the unit is correct, the wavelength is appropriate for radiowaves Check: Solve: ∙ = c, 1 MHz = 10 6 s −1 Conceptual Plan: Relationships: = 100.7 MHz, (m) Given: Find: (MHz) (s −1 ) (m) 14 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Color The color of light is determined by its wavelength or frequency White light is a mixture of all the colors of visible light a spectrum RedOrangeYellowGreenBlueViolet When an object absorbs some of the wavelengths of white light and reflects others, it appears colored the observed color is predominantly the colors reflected 15 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Amplitude & Wavelength 16 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Electromagnetic Spectrum Visible light comprises only a small fraction of all the wavelengths of light – called the electromagnetic spectrum Shorter wavelength (high-frequency) light has higher energy radiowave light has the lowest energy gamma ray light has the highest energy High-energy electromagnetic radiation can potentially damage biological molecules ionizing radiation 17 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Types of Electromagnetic Radiation low frequency and energy high frequency and energy 18 Tro: Chemistry: A Molecular Approach, 2/e Electromagnetic waves are classified by their wavelength Radiowaves = > 0.01 m Microwaves = 10 −4 < < 10 −2 m Infrared (IR) far = 10 −5 < < 10 −4 m middle = 2 x 10 −6 < < 10 −5 m near = 8 x 10 −7 < < 2 x 10 −6 m Visible = 4 x 10 −7 < < 8 x 10 −7 m ROYGBIV Ultraviolet (UV) near = 2 x 10 −7 < < 4 x 10 −7 m far = 1 x 10 −8 < < 2 x 10 −7 m X-rays = 10 −10 < < 10 −8 m Gamma rays = < 10 −10
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Electromagnetic Spectrum 19 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Continuous Spectrum 20 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Thermal Imaging using Infrared Light 21 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Sunburns Caused by High-Energy UV Radiation 22 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Using High-Energy Radiation to Kill Cancer Cells 23 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Interference The interaction between waves is called interference When waves interact so that they add to make a larger wave it is called constructive interference waves are in-phase When waves interact so they cancel each other it is called destructive interference waves are out-of-phase 24 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Interference 25 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Diffraction When traveling waves encounter an obstacle or opening in a barrier that is about the same size as the wavelength, they bend around it – this is called diffraction traveling particles do not diffract The diffraction of light through two slits separated by a distance comparable to the wavelength results in an interference pattern of the diffracted waves An interference pattern is a characteristic of all light waves 26 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Diffraction 27 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e 2-Slit Interference 28 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Photoelectric Effect It was observed that many metals emit electrons when a light shines on their surface this is called the photoelectric effect Classic wave theory attributed this effect to the light energy being transferred to the electron According to this theory, if the wavelength of light is made shorter, or the light waves’ intensity made brighter, more electrons should be ejected remember: the energy of a wave is directly proportional to its amplitude and its frequency this idea predicts if a dim light were used there would be a lag time before electrons were emitted to give the electrons time to absorb enough energy 29 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Photoelectric Effect 30 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Photoelectric Effect: The Problem In experiments it was observed that there was a minimum frequency needed before electrons would be emitted called the threshold frequency regardless of the intensity It was also observed that high-frequency light from a dim source caused electron emission without any lag time 31 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Einstein’s Explanation Einstein proposed that the light energy was delivered to the atoms in packets, called quanta or photons The energy of a photon of light is directly proportional to its frequency inversely proportional to its wavelength the proportionality constant is called Planck’s Constant, (h) and has the value 6.626 x 10 −34 J∙s 32 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Example 7.2: Calculate the number of photons in a laser pulse with wavelength 337 nm and total energy 3.83 mJ Solve: E=hc/, 1 nm = 10 −9 m, 1 mJ = 10 −3 J, E total =E photon # photons Conceptual Plan: Relationships: = 337 nm, E pulse = 3.83 mJ number of photons Given: Find: (nm) (m) E photon number photons 33 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Practice – What is the frequency of radiation required to supply 1.0 x 10 2 J of energy from 8.5 x 10 27 photons? 34 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e 35 Practice – What is the frequency of radiation required to supply 1.0 x 10 2 J of energy from 8.5 x 10 27 photons? Solve: E=h, E total = E photon ∙# photons Conceptual Plan: Relationships: E total = 1.0 x 10 2 J, number of photons = 8.5 x 10 27 Given: Find: (s −1 ) E photon number photons Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Practice – Order the following types of electromagnetic radiation: microwaves, gamma rays, green light, red light, ultraviolet light By wavelength (short to long) By frequency (low to high) By energy (least to most) gamma < UV < green < red < microwaves microwaves < red < green < UV < gamma 36 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Ejected Electrons One photon at the threshold frequency gives the electron just enough energy for it to escape the atom binding energy, When irradiated with a shorter wavelength photon, the electron absorbs more energy than is necessary to escape This excess energy becomes kinetic energy of the ejected electron Kinetic Energy = E photon – E binding KE = h − 37 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Suppose a metal will eject electrons from its surface when struck by yellow light. What will happen if the surface is struck with ultraviolet light? 1.No electrons would be ejected. 2.Electrons would be ejected, and they would have the same kinetic energy as those ejected by yellow light. 3.Electrons would be ejected, and they would have greater kinetic energy than those ejected by yellow light. 4.Electrons would be ejected, and they would have lower kinetic energy than those ejected by yellow light. 1.No electrons would be ejected. 2.Electrons would be ejected, and they would have the same kinetic energy as those ejected by yellow light. 3.Electrons would be ejected, and they would have greater kinetic energy than those ejected by yellow light. 4.Electrons would be ejected, and they would have lower kinetic energy than those ejected by yellow light. 38Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Spectra When atoms or molecules absorb energy, that energy is often released as light energy fireworks, neon lights, etc. When that emitted light is passed through a prism, a pattern of particular wavelengths of light is seen that is unique to that type of atom or molecule – the pattern is called an emission spectrum non-continuous can be used to identify the material flame tests 39 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Exciting Gas Atoms to Emit Light with Electrical Energy 40 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Identifying Elements with Flame Tests NaKLiBa 41 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Emission Spectra 42 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Examples of Spectra 43 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Emission vs. Absorption Spectra Spectra of Mercury 44 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Rydberg’s Spectrum Analysis Rydberg analyzed the spectrum of hydrogen and found that it could be described with an equation that involved an inverse square of integers Johannes Rydberg (1854–1919) 45 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Rutherford’s Nuclear Model The atom contains a tiny dense center called the nucleus the volume is about 1/10 trillionth the volume of the atom The nucleus is essentially the entire mass of the atom The nucleus is positively charged the amount of positive charge balances the negative charge of the electrons The electrons move around in the empty space of the atom surrounding the nucleus 46 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Problems with Rutherford’s Nuclear Model of the Atom Electrons are moving charged particles According to classical physics, moving charged particles give off energy Therefore electrons should constantly be giving off energy should cause the atom to glow! The electrons should lose energy, crash into the nucleus, and the atom should collapse!! but it doesn’t! 47 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Bohr Model of the Atom The nuclear model of the atom does not explain what structural changes occur when the atom gains or loses energy Bohr developed a model of the atom to explain how the structure of the atom changes when it undergoes energy transitions Bohr’s major idea was that the energy of the atom was quantized, and that the amount of energy in the atom was related to the electron’s position in the atom quantized means that the atom could only have very specific amounts of energy Neils Bohr (1885–1962) 48 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Bohr’s Model The electrons travel in orbits that are at a fixed distance from the nucleus stationary states therefore the energy of the electron was proportional to the distance the orbit was from the nucleus Electrons emit radiation when they “jump” from an orbit with higher energy down to an orbit with lower energy the emitted radiation was a photon of light the distance between the orbits determined the energy of the photon of light produced 49 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Bohr Model of H Atoms 50 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Wave Behavior of Electrons de Broglie proposed that particles could have wave-like character de Broglie predicted that the wavelength of a particle was inversely proportional to its momentum Because it is so small, the wave character of electrons is significant Louis de Broglie (1892–1987) 51 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Electron Diffraction Proof that the electron had wave nature came a few years later with the demonstration that a beam of electrons would produce an interference pattern as waves do 52 If electrons behave only like particles, there should only be two bright spots on the target However, electrons actually present an interference pattern, demonstrating they behave like waves Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Solve: Example 7.4: Calculate the wavelength of an electron traveling at 2.65 x 10 6 m/s =h/mv Conceptual Plan: Relationships: v = 2.65 x 10 6 m/s, m = 9.11 x 10 −31 kg (back leaf) m Given: Find: m, v (m) 53 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Practice – Determine the wavelength of a neutron traveling at 1.00 x 10 2 m/s (Mass neutron = 1.675 x 10 −24 g) 54 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Solve: Practice – Determine the wavelength of a neutron traveling at 1.00 x 10 2 m/s =h/mv, 1 kg = 10 3 g Conceptual Plan: Relationships: v = 1.00 x 10 2 m/s, m = 1.675 x 10 −24 g m Given: Find: m (kg), v (m) m(g) v = 1.00 x 10 2 m/s, m = 1.675 x 10 −27 kg m 55 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Complementary Properties When you try to observe the wave nature of the electron, you cannot observe its particle nature – and vice-versa wave nature = interference pattern particle nature = position, which slit it is passing through The wave and particle nature of the electron are complementary properties as you know more about one you know less about the other 56 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Uncertainty Principle Heisenberg stated that the product of the uncertainties in both the position and speed of a particle was inversely proportional to its mass x = position, x = uncertainty in position v = velocity, v = uncertainty in velocity m = mass This means that the more accurately you know the position of a small particle, such as an electron, the less you know about its speed and vice-versa 57 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Uncertainty Principle Demonstration Any experiment designed to observe the electron results in detection of a single electron particle and no interference pattern 58 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Determinacy vs. Indeterminacy According to classical physics, particles move in a path determined by the particle’s velocity, position, and forces acting on it determinacy = definite, predictable future Because we cannot know both the position and velocity of an electron, we cannot predict the path it will follow indeterminacy = indefinite future, can only predict probability The best we can do is to describe the probability an electron will be found in a particular region using statistical functions 59 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Trajectory vs. Probability 60 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Electron Energy Electron energy and position are complementary because KE = ½mv 2 For an electron with a given energy, the best we can do is describe a region in the atom of high probability of finding it Many of the properties of atoms are related to the energies of the electrons 61 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Schrödinger’s Equation Schödinger’s Equation allows us to calculate the probability of finding an electron with a particular amount of energy at a particular location in the atom Solutions to Schödinger’s Equation produce many wave functions, A plot of distance vs. 2 represents an orbital, a probability distribution map of a region where the electron is likely to be found 62 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Solutions to the Wave Function, Calculations show that the size, shape, and orientation in space of an orbital are determined to be three integer terms in the wave function added to quantize the energy of the electron These integers are called quantum numbers principal quantum number, n angular momentum quantum number, l magnetic quantum number, m l 63 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Principal Quantum Number, n Characterizes the energy of the electron in a particular orbital corresponds to Bohr’s energy level n can be any integer 1 The larger the value of n, the more energy the orbital has Energies are defined as being negative an electron would have E = 0 when it just escapes the atom The larger the value of n, the larger the orbital As n gets larger, the amount of energy between orbitals gets smaller 64 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Principal Energy Levels in Hydrogen 65 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Angular Momentum Quantum Number, l The angular momentum quantum number determines the shape of the orbital l can have integer values from 0 to (n – 1) Each value of l is called by a particular letter that designates the shape of the orbital s orbitals are spherical p orbitals are like two balloons tied at the knots d orbitals are mainly like four balloons tied at the knot f orbitals are mainly like eight balloons tied at the knot 66 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Magnetic Quantum Number, m l The magnetic quantum number is an integer that specifies the orientation of the orbital the direction in space the orbital is aligned relative to the other orbitals Values are integers from −l to +l including zero gives the number of orbitals of a particular shape when l = 2, the values of m l are −2, −1, 0, +1, +2; which means there are five orbitals with l = 2 67 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Describing an Orbital Each set of n, l, and m l describes one orbital Orbitals with the same value of n are in the same principal energy level aka principal shell Orbitals with the same values of n and l are said to be in the same sublevel aka subshell 68 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Energy Shells and Subshells 69 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Solve: Example 7.5: What are the quantum numbers and names (for example, 2s, 2p) of the orbitals in the n = 4 principal level? How many orbitals exist? l: 0 → (n − 1); m l : −l → +l Conceptual Plan: Relationships: n = 4 orbital designations, number of orbitals Given: Find: nl 70 mlml 0 → (n − 1)−l → +l n = 4 l : 0, 1, 2, 3 n = 4, l = 0 (s) m l : 0 1 orbital 4s n = 4, l = 1 (p) m l : −1,0,+1 3 orbitals 4p n = 4, l = 2 (d) m l : −2,−1,0,+1,+2 5 orbitals 4d n = 4, l = 3 (f) m l : −3,−2,−1,0,+1,+2,+3 7 orbitals 4f total of 16 orbitals: 1 + 3 + 5 + 7 = 4 2 : n 2 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Quantum Mechanical Explanation of Atomic Spectra Each wavelength in the spectrum of an atom corresponds to an electron transition between orbitals When an electron is excited, it transitions from an orbital in a lower energy level to an orbital in a higher energy level When an electron relaxes, it transitions from an orbital in a higher energy level to an orbital in a lower energy level When an electron relaxes, a photon of light is released whose energy equals the energy difference between the orbitals 71 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Electron Transitions To transition to a higher energy state, the electron must gain the correct amount of energy corresponding to the difference in energy between the final and initial states Electrons in high energy states are unstable and tend to lose energy and transition to lower energy states Each line in the emission spectrum corresponds to the difference in energy between two energy states 72 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Quantum Leaps 73 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Predicting the Spectrum of Hydrogen The wavelengths of lines in the emission spectrum of hydrogen can be predicted by calculating the difference in energy between any two states For an electron in energy state n, there are (n – 1) energy states it can transition to, therefore (n – 1) lines it can generate Both the Bohr and Quantum Mechanical Models can predict these lines very accurately for a 1-electron system 74 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Energy Transitions in Hydrogen The energy of a photon released is equal to the difference in energy between the two levels the electron is jumping between It can be calculated by subtracting the energy of the initial state from the energy of the final state E emitted photon = − E electron E electron = E final state − E initial state 75 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Hydrogen Energy Transitions 76 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Solve: 77 Example 7.7: Calculate the wavelength of light emitted when the hydrogen electron transitions from n = 6 to n = 5 E = hc/ E n = −2.18 x 10 −18 J (1/n 2 ) Conceptual Plan: Relationships: n i = 6, n f = 5 m Given: Find: n i, n f E atom E photon E atom = −E photon E photon = −(−2.6644 x 10 −20 J) = 2.6644 x 10 −20 J the unit is correct, the wavelength is in the infrared, which is appropriate because it is less energy than 4→2 (in the visible) Check: Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Practice – Calculate the wavelength of light emitted when the hydrogen electron transitions from n = 2 to n = 1 78 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Solve: Calculate the wavelength of light emitted when the hydrogen electron transitions from n = 2 to n = 1 E = hc/ E n = −2.18 x 10 −18 J (1/n 2 ) Conceptual Plan: Relationships: n i = 2, n f = 1 m Given: Find: n i, n f E atom E photon E atom = −E photon E photon = −(−1.64 x 10 −18 J) = 1.64 x 10 −18 J the unit is correct, the wavelength is in the UV, which is appropriate because it is more energy than 3→2 (in the visible) Check: 79 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Probability & Radial Distribution Functions 2 is the probability density the probability of finding an electron at a particular point in space for s orbital maximum at the nucleus? decreases as you move away from the nucleus The Radial Distribution function represents the total probability at a certain distance from the nucleus maximum at most probable radius Nodes in the functions are where the probability drops to 0 80 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Probability Density Function The probability density function represents the total probability of finding an electron at a particular point in space 81 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Radial Distribution Function The radial distribution function represents the total probability of finding an electron within a thin spherical shell at a distance r from the nucleus The probability at a point decreases with increasing distance from the nucleus, but the volume of the spherical shell increases The net result is a plot that indicates the most probable distance of the electron in a 1s orbital of H is 52.9 pm 82 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e 2s and 3s 2s n = 2, l = 0 3s n = 3, l = 0 83 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Shapes of Atomic Orbitals The l quantum number primarily determines the shape of the orbital l can have integer values from 0 to (n – 1) Each value of l is called by a particular letter that designates the shape of the orbital s orbitals are spherical p orbitals are like two balloons tied at the knots d orbitals are mainly like four balloons tied at the knot f orbitals are mainly like eight balloons tied at the knot 84 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e l = 0, the s orbital Each principal energy level has one s orbital Lowest energy orbital in a principal energy state Spherical Number of nodes = (n – 1) 85 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e l = 1, p orbitals Each principal energy state above n = 1 has three p orbitals m l = −1, 0, +1 Each of the three orbitals points along a different axis p x, p y, p z 2 nd lowest energy orbitals in a principal energy state Two-lobed One node at the nucleus, total of n nodes 86 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e p orbitals 87 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e l = 2, d orbitals Each principal energy state above n = 2 has five d orbitals m l = −2, − 1, 0, +1, +2 Four of the five orbitals are aligned in a different plane the fifth is aligned with the z axis, d z squared d xy, d yz, d xz, d x squared – y squared 3 rd lowest energy orbitals in a principal energy level Mainly four-lobed one is two-lobed with a toroid Planar nodes higher principal levels also have spherical nodes 88 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e d orbitals 89 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e l = 3, f orbitals Each principal energy state above n = 3 has seven d orbitals m l = −3, −2, −1, 0, +1, +2, +3 4 th lowest energy orbitals in a principal energy state Mainly eight-lobed some two-lobed with a toroid Planar nodes higher principal levels also have spherical nodes 90 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e f orbitals 91 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Why are Atoms Spherical? 92 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e The Phase of an Orbital Orbitals are determined from mathematical wave functions A wave function can have positive or negative values as well as nodes where the wave function = 0 The sign of the wave function is called its phase When orbitals interact, their wave functions may be in-phase (same sign) or out-of-phase (opposite signs) this is important in bonding as will be examined in a later chapter 93 Tro: Chemistry: A Molecular Approach, 2/e
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Copyright 2011 Pearson Education, Inc. Tro: Chemistry: A Molecular Approach, 2/e Phases 94 Tro: Chemistry: A Molecular Approach, 2/e
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