An electron jumps from the 4th orbit to the 2nd orbit of hydrogen atom. Given the Rydberg’s constant R = 107 m-1. The frequency in Hz of the emitted radiation is (c = 3x108 m/s)
\(\frac {9}{16}\) x 1015
\(\frac {3}{16}\) x 105
\(\frac {3}{16}\) x 1015
\(\frac {9}{16}\) x 105
The frequency of the emitted radiation can be determined using the Rydberg formula for the hydrogen atom:
\(\frac {1}{λ}\) = R (\(\frac {1}{n_1^2}\) - \(\frac {1}{n_2^2}\))
We know that
ν = \(\frac {c}{λ}\)
Substituting the given values into the Rydberg formula:
\(\frac {1}{λ}\) = R (\(\frac {1}{2^2}\) - \(\frac {1}{4^2}\))
Simplifying:
\(\frac {1}{λ}\) = R (\(\frac {1}{4}\) - \(\frac {1}{16}\))
\(\frac {1}{λ}\) = R x \(\frac {3}{16}\)
Now, let's substitute the value of the Rydberg constant, R = 107 m⁻¹:
\(\frac {1}{λ}\) = (107 m⁻¹) x \(\frac {3}{16}\)
\(\frac {1}{λ}\) = \(\frac {3 \times 10^7}{16}\) m⁻¹
Taking the reciprocal of λ:
λ = \(\frac {16}{3 \times 10^7}\) m
Now, let's calculate the frequency ν: ν = c / λ
ν = \(\frac {(3 \times 10^8 m/s)}{(16 / (3 \times 10^7) m)}\)
ν = \(\frac {9}{16}\) x 1015 Hz
Therefore, the frequency of the emitted radiation is (A) \(\frac {9}{16}\) × 1015 Hz.
In Bohr model of hydrogen atom, if the difference between the radii of \( n^{th} \) and\( (n+1)^{th} \)orbits is equal to the radius of the \( (n-1)^{th} \) orbit, then the value of \( n \) is: