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For the hydrogen spectrum last line of t...

For the hydrogen spectrum last line of the lyman series has frequency v1 last line of lyman series of `He^(+)` ions has frequency `V_(2)` and `1^(st)` line of Lyman series of `He^(+)` ions has frequency `v_(3)` then

A

`4 v_(1)=v_(2)+v_(3)`

B

`v_(1)=4v_(2)+v_(3)`

C

`v_(2)=v_(3)-v_(1)`

D

`v_(2)=v_(1)+v_(3)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the relationships between the frequencies of the last line of the Lyman series for hydrogen and the He\(^+\) ion. We will denote the frequencies as follows: - \( \nu_1 \): Last line of the Lyman series for hydrogen - \( \nu_2 \): Last line of the Lyman series for He\(^+\) ion - \( \nu_3 \): First line of the Lyman series for He\(^+\) ion ### Step 1: Calculate \( \nu_1 \) for Hydrogen The frequency of the last line of the Lyman series for hydrogen can be calculated using the Rydberg formula: \[ \nu_1 = R_H \cdot c \cdot \left(1 - \frac{1}{\infty^2}\right) \] Where: - \( R_H \) is the Rydberg constant for hydrogen - \( c \) is the speed of light Since \( n_1 = 1 \) and \( n_2 = \infty \): \[ \nu_1 = R_H \cdot c \cdot (1 - 0) = R_H \cdot c \] ### Step 2: Calculate \( \nu_2 \) for He\(^+\) For the He\(^+\) ion, the last line of the Lyman series can be calculated similarly, but with \( Z = 2 \): \[ \nu_2 = R_H \cdot Z^2 \cdot c \cdot \left(1 - \frac{1}{\infty^2}\right) \] Substituting \( Z = 2 \): \[ \nu_2 = R_H \cdot (2^2) \cdot c \cdot (1 - 0) = 4R_H \cdot c \] ### Step 3: Calculate \( \nu_3 \) for He\(^+\) For the first line of the Lyman series for He\(^+\), we have \( n_1 = 1 \) and \( n_2 = 2 \): \[ \nu_3 = R_H \cdot Z^2 \cdot c \cdot \left(1 - \frac{1}{2^2}\right) \] Substituting \( Z = 2 \): \[ \nu_3 = R_H \cdot (2^2) \cdot c \cdot \left(1 - \frac{1}{4}\right) = 4R_H \cdot c \cdot \left(\frac{3}{4}\right) = 3R_H \cdot c \] ### Step 4: Establish the relationship between \( \nu_1 \), \( \nu_2 \), and \( \nu_3 \) Now we have: - \( \nu_1 = R_H \cdot c \) - \( \nu_2 = 4R_H \cdot c \) - \( \nu_3 = 3R_H \cdot c \) We can express the relationship between these frequencies: \[ \nu_2 = \nu_1 + \nu_3 \] Substituting the values: \[ 4R_H \cdot c = R_H \cdot c + 3R_H \cdot c \] This simplifies to: \[ 4R_H \cdot c = 4R_H \cdot c \] This confirms that the relationship holds true. ### Conclusion The relationship between the frequencies is: \[ \nu_2 = \nu_1 + \nu_3 \] Thus, the correct option is the one that states this relationship.
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