We are given the equation for the de-Broglie wavelength:
\[ \lambda = \frac{h}{\sqrt{2mE}}. \]
From this equation, rearranging to solve for \( h \):
\[ h = \lambda \sqrt{2mE}. \]
Now, let's find the dimensional formula for \( h \):
Now, substitute these into the equation:
\[ [h] = [L] \times \sqrt{[M] \times [ML^2T^{-2}]}. \]
Simplifying the terms inside the square root:
\[ [h] = [L] \times \sqrt{[M] \times [M][L^2][T^{-2}]} = [L] \times \sqrt{[M^2L^2T^{-2}]} = [L] \times [MLT^{-1}]. \]
Thus, the dimensional formula for \( h \) is:
\[ [h] = [ML^2T^{-1}]. \]
Therefore, the correct answer is Option (2).
Statement-1: \( \text{ClF}_3 \) has 3 possible structures.
Statement-2: \( \text{III} \) is the most stable structure due to least lone pair-bond pair (lp-bp) repulsion.
Which of the following options is correct?
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is: