Regarding the molecular orbital (MO) energy levels for homonuclear diatomic molecules, the INCORRECT statement(s) is (are):
Bond length of \( \text{Li}_2 \) is larger than the bond length of \( \text{B}_2 \)
(A) Bond order of \( \text{Ne}_2 \) is zero
Electronic configuration of \( \text{Ne}_2 \): 10 bonding and 10 antibonding electrons.
\[ \text{Bond order} = \frac{10 - 10}{2} = 0 \quad \Rightarrow \text{Correct} \]
(B) HOMO of \( \text{F}_2 \) is \( \sigma \)-type
Electronic configuration of \( \text{F}_2 \) based on MO theory:
\[\sigma_{1s}^2 \, \sigma_{1s}^{*2} \, \sigma_{2s}^2 \, \sigma_{2s}^{*2} \, \sigma_{2p_z}^2 \, \pi_{2p_x}^2 = \pi_{2p_y}^2 \, \pi_{2p_x}^{*1} = \pi_{2p_y}^{*1}\]
So, the HOMO is the \( \pi^* \) orbital — not a \( \sigma \)-type orbital.
\[ \Rightarrow \text{Incorrect} \]
(C) Bond energy of \( \text{O}_2^+ \) is smaller than \( \text{O}_2 \)
Bond order of \( \text{O}_2 \) is 2; for \( \text{O}_2^+ \), one electron is removed from an antibonding orbital, increasing bond order to 2.5.
Since bond energy \( \propto \) bond order:
\[ \text{O}_2^+ \text{ has higher bond energy than } \text{O}_2 \Rightarrow \text{Incorrect} \]
(D) Bond length of \( \text{Li}_2 \) is larger than \( \text{B}_2 \)
Bond length generally increases with the size of the atom. Lithium is a larger atom than boron. So:
\[ \text{Bond length of Li}_2 > \text{Bond length of B}_2 \Rightarrow \text{Correct} \]
Final Answer: \( \boxed{\text{(B), (C)}} \)
Which of the following statement is true with respect to H\(_2\)O, NH\(_3\) and CH\(_4\)?
(A) The central atoms of all the molecules are sp\(^3\) hybridized.
(B) The H–O–H, H–N–H and H–C–H angles in the above molecules are 104.5°, 107.5° and 109.5° respectively.
(C) The increasing order of dipole moment is CH\(_4\)<NH\(_3\)<H\(_2\)O.
(D) Both H\(_2\)O and NH\(_3\) are Lewis acids and CH\(_4\) is a Lewis base.
(E) A solution of NH\(_3\) in H\(_2\)O is basic. In this solution NH\(_3\) and H\(_2\)O act as Lowry-Bronsted acid and base respectively.
Which of the following linear combinations of atomic orbitals will lead to the formation of molecular orbitals in homonuclear diatomic molecules (internuclear axis in z-direction)?
(1) \( 2p_z \) and \( 2p_x \)
(2) \( 2s \) and \( 2p_x \)
(3) \( 3d_{xy} \) and \( 3d_{x^2-y^2} \)
(4) \( 2s \) and \( 2p_z \)
(5) \( 2p_z \) and \( 3d_{x^2-y^2} \)
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
A solid glass sphere of refractive index $ n = \sqrt{3} $ and radius $ R $ contains a spherical air cavity of radius $ \dfrac{R}{2} $, as shown in the figure. A very thin glass layer is present at the point $ O $ so that the air cavity (refractive index $ n = 1 $) remains inside the glass sphere. An unpolarized, unidirectional and monochromatic light source $ S $ emits a light ray from a point inside the glass sphere towards the periphery of the glass sphere. If the light is reflected from the point $ O $ and is fully polarized, then the angle of incidence at the inner surface of the glass sphere is $ \theta $. The value of $ \sin \theta $ is ____
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):
In a scattering experiment, a particle of mass $ 2m $ collides with another particle of mass $ m $, which is initially at rest. Assuming the collision to be perfectly elastic, the maximum angular deviation $ \theta $ of the heavier particle, as shown in the figure, in radians is: