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Lecture 13: Heisenberg and Uncertainty

Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics Suppose the positions and speeds of all particles in the universe are measured

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Page 1: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Lecture 13: Heisenberg and Uncertainty

Page 2: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Determinism of Classical Mechanics

Suppose the positions and speeds of all particles in the universe are measured to sufficient accuracy at a particular instant in time

It is possible to predict the motions of every particle at any time in the future (or in the past for that matter)

“An intelligent being knowing, at a given instant of time, all forcesacting in nature, as well as the momentary positions of all things ofwhich the universe consists, would be able to comprehend themotions of the largest bodies of the world and those of the smallestatoms in one single formula, provided it were sufficiently powerfulto subject all the data to analysis; to it, nothing would be uncertain,both future and past would be present before its eyes.”

Pierre Simon Laplace

Page 3: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Role of an Observer

The observer is objective and passive

Physical events happen independently of whether there is an observer or not

This is known as objective reality

Page 4: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Double-Slit Experiment:cannot predict where electron would land

Page 5: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Double-Slit Experiment:act of observation affects behaviour of electron

Page 6: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Role of an Observer in Quantum Mechanics

The observer is not objective and passive

The act of observation changes the physical system irrevocably

This is known as subjective reality

Page 7: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Heisenberg realised that ...

In the world of very small particles, one cannot measure any property of a particle without interacting with it in some way

This introduces an unavoidable uncertainty into the result

One can never measure all the properties exactly

Werner Heisenberg (1901-1976)

Page 8: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Measuring the position and momentum of an electron

Shine light on electron and detect reflected light using a microscope

Minimum uncertainty in position is given by the wavelength of the light

So to determine the position accurately, it is necessary to use light with a short wavelength

Page 9: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Measuring the position and momentum of an electron (cont’d)

By Planck’s law E = hc/, a photon with a short wavelength has a large energy

Thus, it would impart a large ‘kick’ to the electron

But to determine its momentum accurately, electron must only be given a small kick

This means using light of long wavelength!

Page 10: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Fundamental Trade Off …

Use light with short wavelength:

– accurate measurement of position but not momentum

Use light with long wavelength:

– accurate measurement of momentum but not position

Page 11: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Heisenberg’s Uncertainty Principle

The more accurately you know the position (i.e., the smaller x is) , the less accurately you know the momentum (i.e., the larger p is); and vice versa

applet

Page 12: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Implications

It is impossible to know both the position and momentum exactly, i.e., x=0 and p=0

These uncertainties are inherent in the physical world and have nothing to do with the skill of the observer

Because h is so small, these uncertainties are not observable in normal everyday situations

Page 13: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Example of Baseball

A pitcher throws a 0.1-kg baseball at 40 m/s

So momentum is 0.1 x 40 = 4 kg m/s

Suppose the momentum is measured to an accuracy of 1 percent , i.e.,

p = 0.01 p = 4 x 10-2 kg m/s

Page 14: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Example of Baseball (cont’d)

The uncertainty in position is then

No wonder one does not observe the effects of the uncertainty principle in everyday life!

Page 15: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Example of Electron

Same situation, but baseball replaced by an electron which has mass 9.11 x 10-31 kg

So momentum = 3.6 x 10-29 kg m/s and its uncertainty = 3.6 x 10-31 kg m/s

The uncertainty in position is then

Page 16: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

If Planck’s constant were much larger...

Page 17: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Another Consequence of Heisenberg’s Uncertainty Principle

A quantum particle can never be in a state of rest, as this would mean we know both its position and momentum precisely

Thus, the carriage will be jiggling around thebottom of the valleyforever

Page 18: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Heisenberg’s Uncertainty Principle involving energy and time

The more accurately we know the energy of a body, the less accurately we know how long it possessed that energy

The energy can be known with perfect precision (E =

0), only if the measurement is made over an infinite period of time (t = ∞)

Page 19: Lecture 13: Heisenberg and Uncertainty. Determinism of Classical Mechanics  Suppose the positions and speeds of all particles in the universe are measured

Summary: Lessons from Heisenberg

The idea of a perfectly predictable universe cannot be true

There is no such thing as an ideal, objective observer