Deriving the phase velocity of a wavefunction

In summary, the conversation discusses the derivation of the phase velocity equation +/- v = -(p\Psi / pt) / (p\Psi / px). It is derived by substituting y = t into the equation, and it is shown that letting y = a(t^b) also results in the same equation. This shows the relationship between the phase velocities in the x and y spatial dimensions. The equation is derived by transforming it into terms of x and t, and it is related to the angular frequency and propagation number of the wave. The minus sign in the equation represents the direction of phase propagation.
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buffordboy23
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Homework Statement


If [tex]\Psi[/tex] = f(x, y) and x = g(t), y = h(t), then (d[tex]\Psi[/tex] / dt) = (p[tex]\Psi[/tex] / px)(dx / dt) + (p[tex]\Psi[/tex] / py)(dy / dt), where "p" symbolizes the partial derivative here and throughout the rest of this posting.

Derive the phase velocity equation +/- v = -(p[tex]\Psi[/tex] / pt) / (p[tex]\Psi[/tex] / px)


Homework Equations







The Attempt at a Solution



This answer is given in the back of the book, but I am trying to understand both mathematically and physically about what is happening during this derivation.

The solution: Let y = t, then through substitution the equation is derived.

Question #1: Is let y = at, where a = constant, a better a solution since the result leads to the same derived equation?

Question #2: What happens physically if we let y = a(t^b), where a and b are both constants? Substitution reveals that the grouping of terms with the variable y become b(p[tex]\Psi[/tex] / pt), which leads to the same derived equation but with the right-hand side multiplied by the constant b. This result shows that the phase velocity in the x-spatial dimension relies on the phase velocity in the y-spatial dimension, but can this be? Is this alternate derivation due to superposition of the x- and y-spatial dimension component waveforms?

Question #3: To derive the required equation, I understand that the equation must be transformed into terms of x and t. In deriving the equation using the solution from question one, what are we saying both mathematically and physically about [tex]\Psi[/tex]? I know that [tex]\Psi[/tex] describes a surface wave, and that the absolute value of the expression (p[tex]\Psi[/tex] / pt) equals [tex]\omega[/tex], the angular frequency of the wave, and that the absolute value of (p[tex]\Psi[/tex] / px) = k, the propagation number.
 
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  • #2
Question #4: What is the physical meaning of the minus sign in the derived equation? I think it's the direction of phase propagation, but I'm not sure.
 

What is the phase velocity of a wavefunction?

The phase velocity of a wavefunction is the rate at which the phase of the wave changes in space and time. It is a measure of how quickly the wave is moving and is given by the ratio of the frequency of the wave to its wavelength.

How do you calculate the phase velocity of a wavefunction?

The phase velocity of a wavefunction can be calculated by dividing the frequency of the wave by its wavelength. This can also be represented by the product of the wave's angular frequency and its wavenumber.

What factors affect the phase velocity of a wavefunction?

The phase velocity of a wavefunction is affected by the medium through which the wave is propagating, as well as the properties of the wave itself, such as its frequency and wavelength. The phase velocity is also dependent on the boundary conditions of the system in which the wave is propagating.

What is the relationship between phase velocity and group velocity?

Phase velocity and group velocity are related, but they are not the same. While phase velocity measures the speed at which the phase of the wave is changing, group velocity measures the speed at which the energy or information of the wave is being transmitted. In some cases, the two velocities may be equal, but in other cases, they may differ.

Why is the phase velocity of a wavefunction important in physics?

The phase velocity of a wavefunction is important in physics because it allows us to understand the behavior of waves in different mediums and under different conditions. It also plays a crucial role in various applications, such as telecommunications, where the transmission of information relies on the proper understanding and manipulation of wavefunctions.

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