Machine-translated by Google. Questions are authored in English.
Top

Wave Function and Probability Questions and Answers

1.

A quantum particle is confined in a one-dimensional space of \(0 \le x \le 2\). Consider a normalized wavefunction of the particle as

\[ \psi(x) = \sqrt{p/5}\,[1 + \cos(\pi x/2)] \sin(\pi x/2). \]

Which of the following options gives the correct value of \(p\)?

Exam Year(s)

IIT JAM - 2026,

Answer: C

Normalisation gives \(p = 4\).

The wavefunction must satisfy \(\int_0^2 |\psi|^2 dx = 1\). Substitute \(u = \pi x/2\), so \(dx = \frac{2}{\pi}du\) and \(u\) runs from 0 to \(\pi\):

\[ \begin{aligned} 1 &= \frac{p}{5} \cdot \frac{2}{\pi} \int_0^{\pi} I(u)\, du \\ I(u) &= (1 + \cos u)^{2} \sin^{2} u \end{aligned} \]

Expanding, \((1 + \cos u)^2 \sin^2 u = \sin^2 u + 2\cos u \sin^2 u + \cos^2 u \sin^2 u\). Over 0 to \(\pi\) these integrate to \(\frac{\pi}{2}\), 0 and \(\frac{\pi}{8}\):

\[ \begin{aligned} 1 &= \frac{p}{5} \cdot \frac{2}{\pi} \cdot \frac{5\pi}{8} \\ &= \frac{p}{4}, \quad p = 4 \end{aligned} \]

The middle term vanishes because \(\sin^3 u\) is the same at both limits. The values 1, 2 and 3 would leave the total probability at a quarter, a half or three quarters.

Please log in or register to report this question.

2.

The condition for two distinct quantum mechanical states, represented by wave functions \(\psi_{1}(x)\) and \(\psi_{2}(x)\) respectively, to be orthogonal is :

Exam Year(s)

MH SET - 2018, SET Exam - 2018,

Answer: B

The states are orthogonal when \(\int_{-\infty}^{\infty}\psi_{1}^{*}(x)\psi_{2}(x)\,dx = 0\).

Orthogonality means the inner product of the two wave functions vanishes. For functions of x the inner product is the overlap integral of the complex conjugate of one with the other, so the condition is that this integral is zero. Eigenfunctions of a Hermitian operator belonging to different eigenvalues always satisfy it.

An integral equal to 1 is the normalization condition, which applies when the two functions are the same normalized state. An infinite overlap signals non-normalizable functions, and the symmetric sum set equal to 1 is not a condition of orthogonality at all.

Please log in or register to report this question.

3.

A particle is represented by a plane wave in position space. Its wave function in momentum space is :

Exam Year(s)

MH SET - 2018, SET Exam - 2018,

Answer: A

Its momentum-space wave function is a delta function.

A plane wave \( e^{ip_{0}x/\hbar} \) has one definite momentum \( p_{0} \). Its Fourier transform, the momentum-space wave function, is \( \phi(p) \propto \delta(p - p_{0}) \): all the probability sits at \( p_{0} \). This is the uncertainty principle at its extreme, with \( \Delta x \) infinite and \( \Delta p = 0 \).

A Gaussian in position transforms into a Gaussian in momentum (a wave packet), and a Lorentzian is the transform of an exponentially decaying function. A plane wave transforms into a plane wave only for a delta function in position, the reverse case.

Please log in or register to report this question.

Loading…

Other Subjects

Tags: Wave Function and Probability Questions and Answers || Wave Function and Probability MCQ Questions and Answers || Wave Function and Probability GK Questions and Answers || Wave Function and Probability GK MCQ Questions || Wave Function and Probability Multiple Choice Questions and Answers || Wave Function and Probability GK || GK on Wave Function and Probability || Quantum Mechanics Questions and Answers || Quantum Mechanics MCQ Questions and Answers || Quantum Mechanics GK Questions and Answers || GK on Quantum Mechanics