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Unit 3: Atomic Theory & Quantum Mechanics Sections A.4 – A.5. In which you will learn about: Blackbody Radiation The photoelectric effect Atomic emission spectra The Bohr Model of the Atom. A.4 The Particle Nature of Light. Considering light as a wave explains much of its everyday behavior
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Unit 3: Atomic Theory & Quantum MechanicsSections A.4 – A.5 In which you will learn about: Blackbody Radiation The photoelectric effect Atomic emission spectra The Bohr Model of the Atom
A.4 The Particle Nature of Light • Considering light as a wave explains much of its everyday behavior • It does NOT explain how light interacts with matter. For example… • Doesn’t explain why heated objects only emit certain frequencies of light at a given temperature (blackbody radiation) • Doesn’t explain why some metals emit electrons when light of a specific frequency shines on them (photoelectric effect)
Blackbody Radiation • When objects are heated, they emit glowing light • Temperature = average kinetic energy of particles • As the iron in the picture gets hotter, it possesses a greater amount of energy and emits different colors of light which correspond to different frequencies and wavelengths (red to orange to bluish)
The Quantum Model • The wave model could not explain the emission of these different wavelengths • In 1900, Max Planck (1858-1947) began to research this phenomenon • His results showed that matter can gain or lose energy only in small, specific amounts, called quanta. • Quantum = the minimum amount of energy that can be gained or lost by an atom • Remember, light = electromagnetic radiation = energy.
Why is the quantum idea so weird? • Planck and other physicists of the time thought the concept of quantized energy was revolutionary, and some found it disturbing. • Think of it this way… • You’re heating a cup of water in a microwave • You should be able to add any amount of thermal energy to the water by regulating the power and the time the microwave is on (ok, normal so far…) • Instead, the water’s temperature increases in infinitesimally small steps as its molecules absorb quanta of energy • Because the steps are so small, the temp. rise seems continuous, rather than stepwise
Energy of a Quantum • Quantum = discrete amount of energy = packet of energy = packet of light = photon Ephoton = hν • E = energy • h = Planck’s constant = 6.626 x 10-34 J∙s • ν = frequency • NOTE: J stands for Joule, which is the SI unit for energy • NOTE 2: As energy increases, frequency increases. They are directly proportional.
Quantum Analogy • Think of a child building a wall of wooden blocks • The child can add or take away height from the wall only in increments of whole numbers of blocks • Similarly, matter can only have certain amounts of energy—quantities of energy between these values do not exist • OR, think of a ladder. To climb it, you must place your feet on each rung, but you can’t step up using the space between.
Example Problem - GUESS • Every object gets its color by reflecting a certain portion of incident light. The color is determined by the wavelength of the reflected photons, thus by their energy. What is the energy of a photon from the violet portion of the Sun’s light if it has a frequency of 7.230 x 1014 1/s? • G: ν = 7.230 x 1014 1/s & h = 6.626 x 10-34 J∙s • U: E = ? • E: E = hν • S: E =(6.626 x 10-34 J∙s)(7.230 x 1014 1/s) • S: 4.791 x 10-19 J • This answer makes sense, because although the energy is very small, it is the energy of ONE photon of violet light.
The Photoelectric Effect • Scientists also knew that the wave model of light could not explain a phenomenon called the photoelectric effect. • Photoelectric effect = electrons (called photoelectrons) are emitted from a metal’s surface when light of a certain frequency shines on the surface • This effect does NOT depend on the intensity (brightness of the light) • This effect does NOT depend on how long the light shines • The light MUST be at the threshold frequency or higher for the effect to work • Every metal has it’s own threshold frequency – for example, potassium will eject electrons when green light shines on it, but beryllium will not.
Light’s Dual Nature • To explain the photoelectric effect, Albert Einstein proposed in 1905 that light has a dual nature • A beam of light has wavelike and particle-like properties. • It can be thought of as a beam of bundles of energy called photons. • Photon = mass-less particle that carries a quantum of energy • Einstein calculated that the energy of a photon must have a certain threshold value to cause the ejection of the photoelectron from the surface of the metal. • Even small numbers of photons with energy above the threshold value will cause the photoelectric effect • Einstein won the Nobel Prize in Physics in 1921 for this work (not for E=mc2 or special relativity!)
Wave-Particle Duality • Most people get confused with the idea of light being both a wave and a particle. I think of it like this (must watch this one on the comp!):
Neon Signs • Have you ever wondered how light is produced in the glowing tubes of neon signs? • This process is another phenomenon that cannot be explained by the wave model of light • The light of the neon sign is produced by passing electricity through a tube filled with neon gas. • Neon atoms in the tube absorb energy and become excited (unstable) • These excited atoms return to their stable (ground) state by emitting light to release that energy. • Neon signs only produce red! Other colors that are in “neon” signs are actually different gases.
Atomic Emission Spectra • If the light emitted by the neon is passed through a glass prism, neon’s atomic emission spectrum is produced. • Atomic emission spectrum = the set of frequencies of the electromagnetic waves emitted by atoms of the element (see below for neon’s—3rd from top—spectrum)
What to look for in Atomic Emission Spectra • Neon’s atomic emission spectrum consists of several individual lines of color corresponding to the frequencies of radiation emitted by the atoms of neon • Note that it is NOT a continuous range of colors, such as the spectrum for sunlight (white light). • Each element’s atomic emission spectrum is unique and can be used to identify an element or determine whether that element is part of an unknown compound (we’ll be conducting a lab on this during our next long block!)
A.5 Bohr’s Model of the Atom • The dual wave-particle model of light accounted for several previously unexplainable phenomena, but scientists still did not understand the relationship among atomic structure, electrons, and atomic emission spectra. • Recall the hydrogen’s atomic emission spectrum is discontinuous; that is, it is made up of only certain frequencies of light – WHY?? • Niels Bohr, a Danish physicist working in Rutherford’s laboratory in 1913, proposed a quantum model for the hydrogen atom that seems to answer this question. • His model also correctly predicted the frequencies of the lines in hydrogen’s atomic emission spectrum
Energy States of Hydrogen • Bohr proposed that the hydrogen atom has only certain allowable energy states. • Ground state = the lowest allowable energy state • Excited state = when at atom gains energy, its electrons are in this state
Bohr’s Planetary Model WITH Orbits • Bohr related the hydrogen atom’s energy states to the electron within the atom. • He suggested that the electron in a hydrogen atom moves around the nucleus in only certain allowed circular orbits. • The smaller the electron’s orbit, the lower the atom’s energy state, or energy level. The converse is also true. • Hydrogen can have many different excited states, although it only contains one electron (but it can only have one ground state).
Quantum Numbers • In order to complete his calculations, Bohr assigned a number, n, called a quantum number, to each orbit.
The Hydrogen Line Spectrum • Bohr suggested that the hydrogen atom is in the ground state, also called the first energy level, when its single electron is in the n = 1 orbit. • In the ground state, the atom does not radiate energy. • When energy is added from an outside source, the electron moves to a higher-energy orbit, such as n = 2. • Such an electron transition raises the atom to the excited state. • When the atom is in the excited state, it can drop from the higher-energy orbit to a lower-energy orbit. • As a result of this transition, the atom emits a photon corresponding to the energy difference between the two levels. • ΔE = Ehigher-orbit – Elower-orbit = Ephoton = hν
Hydrogen Further Explained • Because only certain atomic energies are possible, only certain frequencies of electromagnetic radiation can be emitted (hence, the discontinuous lines on the spectrum).
Balmer, Lyman, Paschen Series • In the previous slide, it was shown that the four colored lines in the hydrogen spectrum are a result of the electron moving from energy levels • 6 2 = purple line • 5 2 = blue line • 4 2 = green line • 3 2 = red line • These are the only transitions in the VISIBLE spectrum • Other transitions can occur. If the electron goes from • Excited state 1 = Lyman Series (only seen in UV) • Excited state 2 = Balmer Series (only seen in visible) • Excited state 3 = Paschen Series (only seen in IR)
The Limits of Bohr’s Model • Bohr’s model explained hydrogen’s observed spectral lines • But it failed to explain the spectrum of any other element! (too many electrons to consider) • Bohr’s model also does not account for the chemical behavior of atoms • In fact, although Bohr’s idea of quantized energy levels laid the groundwork for atomic models to come… • Later experiments showed that the Bohr model was fundamentally incorrect! (And now we have to re-teach you everything you ever learned about atoms, isn’t this fun?) • The movements of electrons in atoms are not completely understood even now; however, evidence indicates that electrons do NOT move around the nucleus in circular orbits.
A.4 Homework Questions • 1) Calculate the energy possessed by a single photon of each of the following types of electromagnetic radiation. • a) 6.32 x 1020 1/s • b) 9.50 x 1013 Hz • c) 1.05 x 1016 1/s • 2) The blue color in some fireworks occurs when copper (I) chloride is heated to approximately 1500 K and emits blue light of wavelength 4.50 x 102 nm. How much energy does one photon of this light carry? (HINT: Use both light equations we’ve learned so far!) • CHALLENGE: The microwaves used to heat food have a wavelength of 0.125 m. What is the energy of one photon of the microwave oven?
A.4 Homework Questions Cont’d • 3) Compare the dual nature of light. • 4) Describe the three phenomena that can only be explained by the particle model of light.
A.5 Homework Question • 5) Explain the reason, according to Bohr’s atomic model, why atomic emission spectra contain only certain frequencies of light.