Need of Wave Packet: Schrodinger's Postulate

In summary, Schrodinger postulated that a material particle in motion is equivalent to a wave packet rather than a single wave train because wave packets are spatially localized and have finite integrals, making them normalizable and able to represent the probability of a particle's position. This is necessary to accurately describe the behavior of particles in experiments.
  • #1
roshan2004
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Why Schrodinger postulated that a material particle in motion is equivalent to a wave packet rather than a single wave train?
 
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  • #2
roshan2004 said:
Why Schrodinger postulated that a material particle in motion is equivalent to a wave packet rather than a single wave train?

By "a single wave train" I guess you mean a plane-polarized wave with a perfectly precise wave vector, e.g.:

[tex]\phi\left(x\right) = e^{ikx}[/tex]

The problem with this function is that it has infinite extent, or infinite uncertainty in position space, as required by the HUP, since [tex]\Delta p = 0[/tex] for this choice. That means that the function is not square-integrable, and therefore is not normalizable, and cannot represent a wavefunction that is a solution the Schrodinger equation.
 
  • #3
I am new to quantum mechanics and have just started introductory wave mechanics so can u please explain it to me in simple terms
 
  • #4
Some of this expands on Spectracats post;

A wave-packet is a function that is spatially localised, whereas infinite wave trains continue to the ends of the universe. When we look at an experiment (single-slit diffraction for example), we know that the electrons are spatially localised in some fashion (within the lab, for example), thus we need a wave-packet to describe the position of the particle.

Since wave-functions represent probability, thus they are mathematically constrained in that the integral over all space must = 1. To be normalisable, the integral over all space must be finite. Wave-packets possesses this property, but single wave trains do not.

Claude.
 

1. What is Schrodinger's postulate?

Schrodinger's postulate is a fundamental principle in quantum mechanics that states that the state of a physical system can be described by a mathematical function called a wave function. This wave function evolves over time according to the Schrodinger equation.

2. What is a wave packet?

A wave packet is a localized disturbance or "packet" of energy in a medium, composed of superimposed waves of different frequencies and wavelengths. In the context of quantum mechanics, it refers to a wave function that is localized in space and time, representing a particle with a well-defined position and momentum.

3. Why is the concept of a wave packet important in Schrodinger's postulate?

The concept of a wave packet is important in Schrodinger's postulate because it allows us to describe the behavior of particles in quantum mechanics. Unlike classical mechanics, where particles have well-defined positions and momentums, the wave packet describes the probabilistic nature of particles in the quantum world.

4. What is the need for wave packets in quantum mechanics?

The need for wave packets in quantum mechanics arises from the fact that particles in the quantum world do not behave like classical particles. In classical mechanics, particles have well-defined positions and momentums, but in quantum mechanics, the position and momentum of a particle are described by the wave function, which is a probabilistic distribution. The concept of a wave packet allows us to describe this probabilistic behavior of particles.

5. How does the Schrodinger equation describe the evolution of a wave packet?

The Schrodinger equation is a mathematical equation that describes how the wave function of a particle changes over time. It takes into account the potential energy of the particle and how it affects the wave function. By solving the Schrodinger equation, we can determine how the wave packet evolves over time, giving us information about the position and momentum of the particle at different points in time.

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