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).
If \( \lambda \) and \( K \) are de Broglie wavelength and kinetic energy, respectively, of a particle with constant mass. The correct graphical representation for the particle will be:
Let \( y = f(x) \) be the solution of the differential equation
\[ \frac{dy}{dx} + 3y \tan^2 x + 3y = \sec^2 x \]
such that \( f(0) = \frac{e^3}{3} + 1 \), then \( f\left( \frac{\pi}{4} \right) \) is equal to:
Find the IUPAC name of the compound.
If \( \lim_{x \to 0} \left( \frac{\tan x}{x} \right)^{\frac{1}{x^2}} = p \), then \( 96 \ln p \) is: 32