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3.8 UNCERTAINTY PRINCIPLE II
A particle approach gives the same result

The uncertainty principle can be arrived at from the point of view of the particle prop-
erties of waves as well as from the point of view of the wave properties of particles.
We might want to measure the position and momentum of an object at a certain mo-
ment. To do so, we must touch it with something that will carry the required information
back to us. That is, we must poke it with a stick, shine light on it, or perform some sim-
ilar act. The measurement process itself thus requires that the object be interfered with in
some way. If we consider such interferences in detail, we are led to the same uncertainty
principle as before even without taking into account the wave nature of moving bodies.
Suppose we look at an electron using light of wavelength , as in Fig. 3.17. Each
photon of this light has the momentum h. When one of these photons bounces
off the electron (which must happen if we are to “see” the electron), the electron’s

Wave Properties of Particles 113


Figure 3.16The wave packet that corresponds to a moving packet is a composite of many individ-
ual waves, as in Fig. 3.13. The phase velocities of the individual waves vary with their wave lengths.
As a result, as the particle moves, the wave packet spreads out in space. The narrower the original
wavepacket—that is, the more precisely we know its position at that time—the more it spreads out
because it is made up of a greater span of waves with different phase velocities.

Wave packet
Classical particle

Ψ^2 t^1

t 2

t 3

x

x

x

Ψ^2

Ψ^2

Figure 3.17An electron cannot be observed without changing its momentum.

Original
momentum
of electron Final
momentum
of electron

Reflected
photon

Incident
photon

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