A hypothetical molecule XY has the following properties Reduced mass: $2 \times 10^{-26}$ kg X-Y bond length: 100 pm Force constant of the bond: $8 \times 10^2$ N.m$^{-1}$
This question requires calculating the frequency of radiation needed for a vibrational transition (v = 0 to v = 1) in a diatomic molecule XY. This is determined using the harmonic oscillator model, relating the vibrational frequency to the bond's force constant ($k$) and the molecule's reduced mass ($\mu$).
The vibrational frequency ($\nu$) in Hertz (Hz) is given by:
$ \nu = \frac{1}{2\pi} \sqrt{\frac{k}{\mu}} $
For the transition from v = 0 to v = 1, the energy difference is $\Delta E = h\nu$. The frequency of the absorbed radiation corresponds to this $\nu$. To obtain the frequency in wavenumbers ($\bar{\nu}$, in cm$^{-1}$), we use the formula:
$ \bar{\nu} = \frac{\nu}{c} $
where $c$ is the speed of light.
Note: The X-Y bond length is not required for this calculation.
Substitute the given values into the formula:
$ \nu = \frac{1}{2\pi} \sqrt{\frac{8 \times 10^2 \text{ N m}^{-1}}{2 \times 10^{-26} \text{ kg}}} $
Simplify the expression under the square root:
$ \nu = \frac{1}{2\pi} \sqrt{4 \times 10^{28} \text{ s}^{-2}} $
Calculate the square root:
$ \nu = \frac{1}{2\pi} \times (2 \times 10^{14} \text{ s}^{-1}) = \frac{10^{14}}{\pi} \text{ Hz} $
Use the relationship $\bar{\nu} = \frac{\nu}{c}$:
$ \bar{\nu} = \frac{10^{14}/\pi \text{ Hz}}{3 \times 10^{10} \text{ cm s}^{-1}} $
Simplify the expression:
$ \bar{\nu} = \frac{10^{14}}{3\pi \times 10^{10}} \text{ cm}^{-1} = \frac{10^4}{3\pi} \text{ cm}^{-1} $
Using $\pi \approx 3.14159$:
$ \bar{\nu} \approx \frac{10000}{3 \times 3.14159} \approx \frac{10000}{9.42477} \approx 1061.03 \text{ cm}^{-1} $
The calculated value is approximately 1061.03 cm$^{-1}$. This value closely matches option C.
Final Answer: The final answer is $\boxed{\text{1061.6}}$
Consider the following six vibrational modes:
symmetric stretching of $CO_2$, O-H symmetric stretching of $H_2O$, stretching of HCl, stretching of $H_2$, N-H symmetric stretching of $NH_3$, and bending of $CO_2$.
Among these modes, if k number of modes are IR active but Raman inactive, l number of modes are IR inactive but Raman active, and m number of modes are both IR and Raman active.
k, l, and m, respectively, are