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Exam 3 covers Lecture, Readings, Discussion, HW, Lab
Exam 3 is tonight, Thurs. Dec. 3, 5:30-7 pm, 145 Birge Magnetic dipoles, dipole moments, and torque Magnetic flux, Faraday effect, Lenz’ law Inductors, inductor circuits Electromagnetic waves: Wavelength, freq, speed E&B fields, intensity, power, radiation pressure Polarization Modern Physics (quantum mechanics) Photons & photoelectric effect Bohr atom: Energy levels, absorbing & emitting photons Uncertainty principle Thurs. Dec. 3, 2009 Phy208 Lect. 26
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From Last time… De Broglie wavelength Uncertainty principle
Wavefunction of a particle
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Spatial extent of ‘wave packet’
x = spatial spread of ‘wave packet’ Spatial extent decreases as the spread in included wavelengths increases. Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Wavefunction Quantify this by giving a physical meaning to the wave that describing the particle. This wave is called the wavefunction. Cannot be experimentally measured! But the square of the wavefunction is a physical quantity. It’s value at some point in space is the probability of finding the particle there! Thurs. Dec. 3, 2009 Phy208 Lect. 26
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The wavefunction 2 Particle has a wavefunction (x) x x
dx Very small x-range = probability to find particle in infinitesimal range dx about x Larger x-range = probability to find particle between x1 and x2 Entire x-range particle must be somewhere Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Probability P(heads)=0.5 P(tails)=0.5 P(1)=1/6 P(2)=1/6 etc Heads
0.0 P(heads)=0.5 P(tails)=0.5 1 Probability 0.5 0.0 2 3 4 5 6 1/6 P(1)=1/6 P(2)=1/6 etc Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Discrete vs continuous
6-sided die, unequal prob 0.5 Loaded die Probability 1/6 0.0 1 2 3 4 5 6 Infinite-sided die, all numbers between 1 and 6 “Continuous” probability distribution 1 P(x) 0.5 0.0 2 3 4 5 6 1/6 x Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Example wavefunction 2 What is P(-2<x<-1)? What is (0)?
= fractional area under curve -2 < x < -1 = 1/8 total area -> P = 0.125 What is (0)? = entire area under 2 curve = 1 = (1/2)(base)(height)=22(0)=1 Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Wavefunctions Each quantum state has different wavefunction
Wavefunction shape determined by physical characteristics of system. Different quantum mechanical systems Pendulum (harmonic oscillator) Hydrogen atom Particle in a box Each has differently shaped wavefunctions Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Quantum ‘Particle in a box’
Particle confined to a fixed region of space e.g. ball in a tube- ball moves only along length L Classically, ball bounces back and forth in tube. A classical ‘state’ of the ball. State indexed by speed, momentum=(mass)x(speed), or kinetic energy. Classical: any momentum, energy is possible. Quantum: momenta, energy are quantized L Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Classical vs Quantum Classical: particle bounces back and forth.
Sometimes velocity is to left, sometimes to right L Quantum mechanics: Particle represented by wave: p = mv = h / Different motions: waves traveling left and right Quantum wavefunction: superposition of both at same time Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Quantum version Quantum state is both velocities at the same time
Superposition waves is standing wave, made equally of Wave traveling right ( p = +h/ ) Wave traveling left ( p = - h/ ) Determined by standing wave condition L=n(/2) : One half-wavelength momentum L Quantum wave function: superposition of both motions. Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Different quantum states
p = mv = h / Different speeds correspond to different subject to standing wave condition integer number of half-wavelengths fit in the tube. Wavefunction: n=1 momentum One half-wavelength n=1 n=2 n=2 Two half-wavelengths momentum Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Particle in box question
A particle in a box has a mass m. Its energy is all kinetic = p2/2m. Just saw that momentum in state n is npo. It’s energy levels A. are equally spaced everywhere B. get farther apart at higher energy C. get closer together at higher energy. Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Particle in box energy levels
Quantized momentum Energy = kinetic Or Quantized Energy n=quantum number Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Zero-point motion Lowest energy is not zero
Confined quantum particle cannot be at rest Always some motion Consequency of uncertainty principle p cannot be zero p not exactly known p cannot be exactly zero Comment here about right-hand-side of uncertainty relation. Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Question A particle is in a particular quantum state in a box of length L. The box is now squeezed to a shorter length, L/2. The particle remains in the same quantum state. The energy of the particle is now A. 2 times bigger B. 2 times smaller C. 4 times bigger D. 4 times smaller E. unchanged Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Quantum dot: particle in 3D box
CdSe quantum dots dispersed in hexane (Bawendi group, MIT) Color from photon absorption Determined by energy-level spacing Decreasing particle size Energy level spacing increases as particle size decreases. i.e Video of making CdSe nanocrystals: Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Interpreting the wavefunction
Probability interpretation The square magnitude of the wavefunction ||2 gives the probability of finding the particle at a particular spatial location Wavefunction Probability = (Wavefunction)2 Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Higher energy wave functions
L n p E Wavefunction Probability n=3 n=2 n=1 Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Probability of finding electron
Classically, equally likely to find particle anywhere QM - true on average for high n Zeroes in the probability! Purely quantum, interference effect Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Quantum Corral D. Eigler (IBM)
48 Iron atoms assembled into a circular ring. The ripples inside the ring reflect the electron quantum states of a circular ring (interference effects). Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Particle in box again: 2 dimensions
Motion in x direction Motion in y direction Same velocity (energy), but details of motion are different. Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Quantum Wave Functions
Probability (2D) Ground state: same wavelength (longest) in both x and y Need two quantum #’s, one for x-motion one for y-motion Use a pair (nx, ny) Ground state: (1,1) Wavefunction Probability = (Wavefunction)2 One-dimensional (1D) case Thurs. Dec. 3, 2009 Phy208 Lect. 26
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2D excited states (nx, ny) = (2,1) (nx, ny) = (1,2) These have exactly the same energy, but the probabilities look different. The different states correspond to ball bouncing in x or in y direction. Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Particle in a box What quantum state could this be? A. nx=2, ny=2
B. nx=3, ny=2 C. nx=1, ny=2 Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Next higher energy state
Ball has same bouncing motion in x and in y. Is higher energy than state with motion only in x or only in y. (nx, ny) = (2,2) Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Three dimensions Object can have different velocity (hence wavelength) in x, y, or z directions. Need three quantum numbers to label state (nx, ny , nz) labels each quantum state (a triplet of integers) Each point in three-dimensional space has a probability associated with it. Not enough dimensions to plot probability But can plot a surface of constant probability. Thurs. Dec. 3, 2009 Phy208 Lect. 26
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Particle in 3D box Ground state surface of constant probability
(nx, ny, nz)=(1,1,1) 2D case Thurs. Dec. 3, 2009 Phy208 Lect. 26
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All these states have the same energy, but different probabilities
(121) (112) (211) All these states have the same energy, but different probabilities Thurs. Dec. 3, 2009 Phy208 Lect. 26
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(222) (221) Thurs. Dec. 3, 2009 Phy208 Lect. 26
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3-D particle in box: summary
Three quantum numbers (nx,ny,nz) label each state nx,y,z=1, 2, 3 … (integers starting at 1) Each state has different motion in x, y, z Quantum numbers determine Momentum in each direction: e.g. Energy: Some quantum states have same energy Thurs. Dec. 3, 2009 Phy208 Lect. 26
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