To find the longest wavelength of the spectral lines in the Balmer series, we begin by using the relationship for the energy levels of hydrogen and the transitions involved.
Step 1: Lyman Series
For the Lyman series:
\[ \frac{hc}{\lambda} = -13.6 \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \quad (\text{in eV}), \]
where \( n_1 = 1 \) for the Lyman series and \( n_2 \) varies.
Given the shortest wavelength in the Lyman series:
\[ \lambda_{\text{Lyman}} = 915 \, \text{\AA}. \]
Step 2: Balmer Series
For the Balmer series:
- \( n_1 = 2 \)
- \( n_2 = 3 \) for the longest wavelength transition.
The energy difference for the transition is given by:
\[ \frac{hc}{\lambda_1} = -13.6 \left( \frac{1}{2^2} - \frac{1}{3^2} \right). \]
Calculating:
\[ \frac{hc}{\lambda_1} = -13.6 \left( \frac{1}{4} - \frac{1}{9} \right). \]
Simplifying:
\[ \frac{hc}{\lambda_1} = -13.6 \left( \frac{5}{36} \right). \]
Step 3: Relating the Wavelengths
Using the given data for the Lyman series:
\[ \lambda_1 = \lambda_{\text{Lyman}} \times \frac{36}{5}. \]
Substituting the given value:
\[ \lambda_1 = 915 \times \frac{36}{5} = 6588 \, \text{\AA}. \]
Therefore, the longest wavelength of spectral lines in the Balmer series is \( 6588 \, \text{\AA} \).
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).