Momentum operator for a free particle with a definite momentum and Energy

In summary, the conversation discusses the momentum operator for a free particle with definite momentum and energy, and whether it is the same as the general momentum operator. The justification is given that the momentum is definite and the position must go to infinity, resulting in differentiation with respect to x. It is clarified that the operator does not depend on the wave function, but will give different results for different wave functions. An example of a wave function with definite momentum and energy is also provided.
  • #1
trelek2
88
0
Hi!

I need an explanation:
Is the momentum operator for a free particle with a definite momentum and energy the same as what we know as the momentum operator in general?

Is it just -ih/2PI()*partial/partial_x?

With the justification that since the momentum is definite, delta p is 0, but delta x must go to infinity so differentiating wrt. x gives

(momentum_operator)*wave_func.=momentum*wave func?

If anyone could clarify I'd be grateful:)
 
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  • #2
The operator does not depend on the wave function, but will give a different result on different wave functions.
 
  • #3
I don't understand what do you mean, can you give an example eg. the function with a definite momentum and energy?
 
  • #4
[tex]\Psi(x,t)=A \exp [i(px - Et) / \hbar][/tex]

Apply the momentum operator to it and see what you get. :smile:
 

What is the momentum operator for a free particle with a definite momentum and energy?

The momentum operator for a free particle with a definite momentum and energy is given by the expression p = mv, where p is the momentum, m is the mass of the particle, and v is the velocity. This operator is used in quantum mechanics to describe the behavior of a particle with a specific momentum and energy.

How is the momentum operator related to the energy of a particle?

The momentum operator and the energy operator are related through the de Broglie relation, which states that the wavelength of a particle is inversely proportional to its momentum. This means that the momentum operator and energy operator are essentially two sides of the same coin, with one being dependent on the other.

What is the significance of a particle having a definite momentum and energy?

Having a definite momentum and energy means that the particle is in a well-defined state, and its position and momentum can be predicted with certainty. This is important in quantum mechanics because it allows for the precise measurement and prediction of a particle's behavior.

Can the momentum operator for a free particle with a definite momentum and energy be used for particles with non-zero mass?

Yes, the momentum operator can be used for particles with any non-zero mass. However, it is important to note that for particles with non-zero mass, the velocity and momentum are not always directly proportional, as they are for massless particles such as photons.

How does the momentum operator for a free particle with a definite momentum and energy relate to the Heisenberg uncertainty principle?

The Heisenberg uncertainty principle states that it is impossible to know both the position and momentum of a particle with perfect accuracy. This means that the momentum operator for a free particle with a definite momentum and energy can only give a range of possible values for the momentum, rather than a precise value. This is a fundamental principle of quantum mechanics and has important implications for the behavior of particles at the subatomic level.

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