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I. Waves & Particles Ch. 4 - Electrons in Atoms
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Light and Electrons zBecause light and electrons have common properties, understanding one helps to understand the other.
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Electromagnetic radiation zEnergy that exhibits wave-like behavior as it travels zIncludes: gamma rays, X-rays, infrared, visible spectrum, microwaves, ultraviolet rays, radio and TV waves
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EM Spectrum LOWENERGYLOWENERGY HIGHENERGYHIGHENERGY
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LOWENERGYLOWENERGY HIGHENERGYHIGHENERGY ROYG.BIV redorangeyellowgreenblueindigoviolet
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Waves zWavelength ( ) - length of one complete wave (measured in m, cm, nm) zFrequency ( ) - # of waves that pass a point during a certain time period yhertz (Hz) = 1/s (s -1 ) zAmplitude (A) - distance from the origin to the trough or crest
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Waves A greater amplitude (intensity) greater frequency (color) crest origin trough A
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EM Spectrum zFrequency & wavelength are inversely proportional c = c:speed of light (3.00 10 8 m/s) :wavelength (m, nm, etc.) :frequency (Hz)
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EM Spectrum GIVEN: = 7.50 x !0 12 Hz = ? c = 3.00 10 8 m/s WORK : = c = 3.00 10 8 m/s 7.50 10 12 Hz = 4.00 10 -5 m zEX: Calculate the wavelength of radiation whose frequency is 7.50 x !0 12 Hz.
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Light as Particles zA property which could not be explained in terms of waves was a phenomenon known as the photoelectric effect – refers to the emission of electrons from a metal when heated or lit.
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Quantum Theory zPlanck (1900) yObserved - emission of light from hot objects yConcluded - energy is emitted in small, specific amounts (quanta) yQuantum - minimum amount of energy change
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Quantum Theory zPlanck (1900) vs. Classical TheoryQuantum Theory
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E:energy (J, joules) h:Planck’s constant (6.6262 10 -34 J·s) :frequency (Hz) E = h zThe energy of a photon is proportional to its frequency.
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Quantum Theory GIVEN: E = ? = 3.55 10 17 Hz h = 6.6262 10 -34 J·s WORK : E = h E = ( 6.6262 10 -34 J·s ) ( 3.55 10 17 Hz ) E = 2.35 10 -16 J zEX: Find the energy of a photon with a frequency of 3.55 10 17 Hz.
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Quantum Theory zEinstein (1905) yObserved - photoelectric effect
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Quantum Theory zEinstein (1905) yConcluded - light has properties of both waves and particles “wave-particle duality” yPhoton - particle of light, having zero mass, carrying a quantum of energy
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Quantum Theory zRadiation is emitted and absorbed only in whole numbers of photons
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II. Bohr Model of the Atom Ch. 4 - Electrons in Atoms
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A. Line-Emission Spectrum ground state excited state ENERGY IN PHOTON OUT
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B. Bohr Model zLinked the atom’s electron with photon emission ze - exist only in paths, or orbits, with specific amounts of energy called energy levels zTherefore… ye - can only gain or lose certain amounts of energy yonly certain photons are produced
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B. Bohr Model 1 2 3 4 5 6 zEnergy of photon depends on the difference in energy levels ze - jumps up when energy is absorbed- gives off light when is falls back down
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C. Other Elements zEach element has a unique bright-line emission spectrum. y“Atomic Fingerprint” Helium zBohr’s calculations only worked for hydrogen!
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zBohr’s model of the atom explained electrons as particles.
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A. Electrons as Waves zLouis de Broglie (1924) yApplied wave-particle theory to e - ye - exhibit wave properties
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B. Quantum Mechanics zHeisenberg Uncertainty Principle yImpossible to know both the velocity and position of an electron at the same time
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B. Quantum Mechanics zSchrödinger Wave Equation (1926) ytreated e- moving around the nucleus as waves ydefines probability of finding an e - ydefines mathematically the wave properties of electrons
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B. Quantum Mechanics Radial Distribution Curve Orbital zOrbital (“electron cloud”) yRegion in space where there is 90% probability of finding an e -
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