The correct option with regard to the following statements is
(a) Time-independent Schrödinger equation can be exactly solved for Be\(^{2+}\).
(b) For a particle confined in a one-dimensional box of length \( l \) with infinite potential barriers, the trial variation function \( \phi = \left[ \left( \frac{3}{l^3} \right)^{1/2} x \right] \) is not an acceptable trial wavefunction for \( 0 \le x \le l \).
(c) Wavefunctions for system of Fermions must be anti-symmetric with respect to exchange of any two Fermions in the system.
(d) Born-Oppenheimer approximation can be used to separate the vibrational and rotational motion of a molecule.
(a) Time-independent Schrödinger equation can be exactly solved for Be2+.
Be2+ has an electronic configuration of 1s2, meaning it has two electrons.
The time-independent Schrödinger equation can be solved exactly only for one-electron systems.
For systems with two or more electrons, the electron-electron interaction term makes it impossible to obtain an exact analytical solution.
We rely on approximation methods like Hartree-Fock.
Therefore, statement (a) is False.
(b) For a particle confined in a one-dimensional box of length l with infinite potential barriers, the trial variation function
φ(x) = [(3/l3)1/2] × x is not an acceptable trial wavefunction for 0 ≤ x ≤ l.
For a trial wavefunction to be acceptable in the variational method for a 1D box with infinite barriers at x = 0 and x = l, it must satisfy the boundary conditions: φ(0) = 0 and φ(l) = 0.
Given: φ(x) = (3/l3)1/2 × x
At x = 0: φ(0) = 0 — boundary condition satisfied.
At x = l: φ(l) = (3/l)1/2 ≠ 0 — boundary condition not satisfied.
Therefore, statement (b) is True.
(c) Wavefunctions for a system of Fermions must be anti-symmetric with respect to exchange of any two Fermions in the system.
Fermions are particles with half-integer spin.
The total wavefunction of a system of identical fermions must be anti-symmetric under exchange — this is the Pauli Exclusion Principle.
Therefore, statement (c) is True.
(d) Born-Oppenheimer approximation can be used to separate the vibrational and rotational motion of a molecule.
The Born-Oppenheimer approximation separates electronic and nuclear motion (not directly vibration and rotation).
Separation of vibrational and rotational motion is a further approximation based on treating the nuclei as a semi-rigid rotor.
Therefore, statement (d) is False.
Summary:
(a) False
(b) True
(c) True
(d) False
\[ \boxed{\text{Correct option is (C)}} \]
Wavefunctions and energies for a particle confined in a cubic box are \( \psi_{n_x,n_y,n_z} \) and \( E_{n_x,n_y,n_z} \), respectively. The functions \( \phi_1, \phi_2, \phi_3 \), and \( \phi_4 \) are written as linear combinations of \( \psi_{n_x,n_y,n_z} \). Among these functions, the eigenfunction(s) of the Hamiltonian operator for this particle is/are \[ \phi_1 = \frac{1}{\sqrt{2}} \psi_{1,4,1} - \frac{1}{\sqrt{2}} \psi_{2,2,3} \] \[ \phi_2 = \frac{1}{\sqrt{2}} \psi_{1,5,1} + \frac{1}{\sqrt{2}} \psi_{3,3,3} \] \[ \phi_3 = \frac{1}{\sqrt{2}} \psi_{1,3,8} + \frac{1}{\sqrt{2}} \psi_{3,8,1} \] \[ \phi_4 = \frac{1}{2} \psi_{3,3,1} + \frac{\sqrt{3}}{2} \psi_{2,4,1} \]
A regular dodecagon (12-sided regular polygon) is inscribed in a circle of radius \( r \) cm as shown in the figure. The side of the dodecagon is \( d \) cm. All the triangles (numbered 1 to 12 in the figure) are used to form squares of side \( r \) cm, and each numbered triangle is used only once to form a square. The number of squares that can be formed and the number of triangles required to form each square, respectively, are:
In the given figure, the numbers associated with the rectangle, triangle, and ellipse are 1, 2, and 3, respectively. Which one among the given options is the most appropriate combination of \( P \), \( Q \), and \( R \)?
The Lineweaver-Burk plot for an enzyme obeying the Michaelis-Menten mechanism is given below.
The slope of the line is \(0.36 \times 10^2\) s, and the y-intercept is \(1.20\) mol\(^{-1}\) L s. The value of the Michaelis constant (\(K_M\)) is ________ \( \times 10^{-3} \) mol L\(^{-1}\) (in integer). [Note: \(v\) is the initial rate, and \([S]_0\) is the substrate concentration]
Consider a Carnot engine with a hot source kept at 500 K. From the hot source, 100 J of energy (heat) is withdrawn at 500 K. The cold sink is kept at 300 K. The efficiency of the Carnot engine is ___________ (rounded off to one decimal place).
For the cell reaction, \[ Hg_2Cl_2 (s) + H_2 (1 \, {atm}) \rightarrow 2Hg (l) + 2H^+ (a=1) + 2Cl^- (a=1) \] The standard cell potential is \( \mathcal{E}^0 = 0.2676 \) V, and \( \left(\frac{\partial \mathcal{E}^0}{\partial T}\right)_P = -3.19 \times 10^{-4} \) V K\(^{-1}\). The standard enthalpy change of the reaction (\( \Delta_r H^0 \)) at 298 K is \( -x \) kJ mol\(^{-1}\). The value of \( x \) is ___________ (rounded off to two decimal places). [Given: Faraday constant \( F = 96500 \) C mol\(^{-1}\)]