BioPHYSICAL chemistry

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An understanding of the properties of biological molecules requires know-
ledge of quantum mechanics. This chapter presents two examples of how
Schrödinger’s equation can be used to solve problems. First, we consider
the one-dimensional particle in a box, in which a particle is trapped inside
a box with infinite walls. The second problem is the simple harmonic
oscillator. For this problem, we consider how quantum mechanics describes
vibrational motion. Using these problems as typical examples, we show
how to use Schrödinger’s equation and discuss how various properties
of objects can be described. In both cases we see that quantum theory
makes surprising predictions, such as tunneling. The usefulness of these
problems is shown by their application to understanding the properties
of conjugated molecules commonly found in biological systems, such as
carotenoids, as well as the vibrational properties of molecules.

One-dimensional particle in a box


A particle of mass mis confined between two walls at x=0 and x=L.
The potential energy is zero inside the box but rises immediately to infinity
at the walls (Figure 10.1). Because the potential is infinite
outside the box, the particle cannot be outside the box
and the wavefunction is zero there. To determine the
properties of the particle inside the box, Schrödinger’s
equation is solved. In this case, the potential energy V(x)
is zero inside of the box, so the equation can be simply
written as:

(10.1)

The solutions to this equation can be written in terms
of exponential, sine, or cosine functions. The choice of

−=

Z^22

2 mx^2 xEx

d
d

ψψ() ()

10 Particle in a box and tunneling


10 Particle in a box and tunneling


V  0

x  0 x  L

V   V  


Figure 10.1
A particle is confined
to be within a box
with a potential of
zero inside the box
and an infinite
potential outside
the box.

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