
How do you calculate ionization energy using Rydberg constant?
Answer
483k+ views
Hint: In this question we have to calculate the wavelength of the absorbed photon by using Rydberg constant. After that we will substitute the value of $ \lambda $ in the Planck energy formula, hence by solving it, we get the value of $ E $ .
The Rydberg equation for absorption is:
$ \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{n_i^2}} - \dfrac{1}{{n_f^2}}} \right) $
Where, $ \lambda $ is the wavelength of the absorbed photon, $ R $ is the Rydberg constant, $ {n_i} $ is the energy level of electron at initial and $ {n_f} $ is the energy level of electron at final.
And,
$ E = \dfrac{{hc}}{\lambda } $
Where, $ E $ is the ionization energy, $ h $ is the Planck constant and $ c $ is the speed of the light, i.e. $ 3 \times {10^8}m{\sec ^{ - 1}} $ .
Complete Step By Step Answer:
By using the Rydberg formula, we can calculate the wavelengths of the spectral line in many elements. The formula was mostly presented as the generalization of the Balmer series for all atomic electron transitions of hydrogen. It was first stated by Johannes Rydberg in $ 1888 $ .
Hence by using the formula of Rydberg which is:
$ \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{n_i^2}} - \dfrac{1}{{n_f^2}}} \right) $
As we know that the electron goes to infinity with respect to the atom, i.e. it leaves the atom while releasing the ionization energy. So, we have $ {n_f} = \infty $ . Assuming that we ionize from the ground state that we have $ {n_i} = 1 $ . So, after substituting these in Rydberg formula we get:
$ \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{n_i^2}} - \dfrac{1}{{n_f^2}}} \right) $
$ \Rightarrow \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{{1^2}}} - \dfrac{1}{\infty }} \right) $
$ \Rightarrow \dfrac{1}{\lambda } = R\left( {1 - 0} \right) $
$ \Rightarrow \dfrac{1}{\lambda } = R $
By substituting this value in Planck energy formula we get:
$ E = \dfrac{{hc}}{\lambda } $
$ \Rightarrow E = hcR $
$ \Rightarrow E = 6.626 \times {10^{ - 34}} \times 3 \times {10^8} \times 1.097 \times {10^7} $
$ \Rightarrow 2.182 \times {10^{ - 18}}J $
Here we are dealing with electrons so the energy should be in $ eV $ . Thus,
$ 1eV = 1.6 \times {10^{ - 19}}J $
Hence, by using this we will convent the value in $ eV $ :
$ E = 2.182 \times {10^{ - 18}}J $
$ \Rightarrow E = \dfrac{{2.182 \times {{10}^{ - 18}}}}{{1.6 \times {{10}^{ - 19}}}} $
$ \Rightarrow E = 13.6eV $
Thus, the ionization energy is $ 13.6eV $ .
Note:
The Rydberg formula generally provides incorrect results for the other spectral transitions in multi-electron atoms. Since the magnitude of the screening of the inner electrons for outer electrons transitions is variable.
The Rydberg equation for absorption is:
$ \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{n_i^2}} - \dfrac{1}{{n_f^2}}} \right) $
Where, $ \lambda $ is the wavelength of the absorbed photon, $ R $ is the Rydberg constant, $ {n_i} $ is the energy level of electron at initial and $ {n_f} $ is the energy level of electron at final.
And,
$ E = \dfrac{{hc}}{\lambda } $
Where, $ E $ is the ionization energy, $ h $ is the Planck constant and $ c $ is the speed of the light, i.e. $ 3 \times {10^8}m{\sec ^{ - 1}} $ .
Complete Step By Step Answer:
By using the Rydberg formula, we can calculate the wavelengths of the spectral line in many elements. The formula was mostly presented as the generalization of the Balmer series for all atomic electron transitions of hydrogen. It was first stated by Johannes Rydberg in $ 1888 $ .
Hence by using the formula of Rydberg which is:
$ \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{n_i^2}} - \dfrac{1}{{n_f^2}}} \right) $
As we know that the electron goes to infinity with respect to the atom, i.e. it leaves the atom while releasing the ionization energy. So, we have $ {n_f} = \infty $ . Assuming that we ionize from the ground state that we have $ {n_i} = 1 $ . So, after substituting these in Rydberg formula we get:
$ \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{n_i^2}} - \dfrac{1}{{n_f^2}}} \right) $
$ \Rightarrow \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{{1^2}}} - \dfrac{1}{\infty }} \right) $
$ \Rightarrow \dfrac{1}{\lambda } = R\left( {1 - 0} \right) $
$ \Rightarrow \dfrac{1}{\lambda } = R $
By substituting this value in Planck energy formula we get:
$ E = \dfrac{{hc}}{\lambda } $
$ \Rightarrow E = hcR $
$ \Rightarrow E = 6.626 \times {10^{ - 34}} \times 3 \times {10^8} \times 1.097 \times {10^7} $
$ \Rightarrow 2.182 \times {10^{ - 18}}J $
Here we are dealing with electrons so the energy should be in $ eV $ . Thus,
$ 1eV = 1.6 \times {10^{ - 19}}J $
Hence, by using this we will convent the value in $ eV $ :
$ E = 2.182 \times {10^{ - 18}}J $
$ \Rightarrow E = \dfrac{{2.182 \times {{10}^{ - 18}}}}{{1.6 \times {{10}^{ - 19}}}} $
$ \Rightarrow E = 13.6eV $
Thus, the ionization energy is $ 13.6eV $ .
Note:
The Rydberg formula generally provides incorrect results for the other spectral transitions in multi-electron atoms. Since the magnitude of the screening of the inner electrons for outer electrons transitions is variable.
Recently Updated Pages
Master Class 11 Business Studies: Engaging Questions & Answers for Success

Master Class 11 English: Engaging Questions & Answers for Success

Master Class 11 Computer Science: Engaging Questions & Answers for Success

Master Class 11 Social Science: Engaging Questions & Answers for Success

Master Class 11 Maths: Engaging Questions & Answers for Success

Master Class 11 Biology: Engaging Questions & Answers for Success

Trending doubts
Differentiate between an exothermic and an endothermic class 11 chemistry CBSE

10 examples of friction in our daily life

One Metric ton is equal to kg A 10000 B 1000 C 100 class 11 physics CBSE

Difference Between Prokaryotic Cells and Eukaryotic Cells

State the laws of reflection of light

Explain zero factorial class 11 maths CBSE

