The energy of a photon emitted during a transition is related to its wavelength by:
\( E = \frac{hc}{\lambda} \)
where \( h \) is Planck's constant, \( c \) is the speed of light, and \( \lambda \) is the wavelength.
From the equation above, we can see that for the shortest wavelength (\( \lambda_{min} \)), the energy (\( E \)) must be maximum.
The energy of a photon emitted during a transition is equal to the difference in energy levels:
\( E = E_{initial} - E_{final} \)
The largest energy difference corresponds to the shortest wavelength. In the given diagram:
The energy levels in a hydrogen atom are given by:
\( E_n = -\frac{13.6 \text{ eV}}{n^2} \)
We can see that transitions C and D are identical in the provided image and diagram, which is likely an error in the original question. Assuming D is meant to be the transition from \( n = 3 \) to \( n = 1 \), D represents the largest energy difference, followed by C (which is the same as D, again suggesting an error), then B, and finally A.
The transition corresponding to the emission of the shortest wavelength is D (assuming it is intended to represent the transition from \( n = 3 \) to \( n = 1 \)) (Option 2).
For \( \alpha, \beta, \gamma \in \mathbb{R} \), if \[ \lim_{x \to 0} \frac{x^2 \sin(\alpha x) + (\gamma - 1)e^{x^2}}{\sin(2x - \beta x)} = 3, \] then \( \beta + \gamma - \alpha \) is equal to:

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by:
If \( S \) and \( S' \) are the foci of the ellipse \[ \frac{x^2}{18} + \frac{y^2}{9} = 1 \] and \( P \) is a point on the ellipse, then \[ \min (SP \cdot S'P) + \max (SP \cdot S'P) \] is equal to: