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For emission line of atomic hydrogen fro...

For emission line of atomic hydrogen from `n_(i)=8` to `n_(f)=n,` the plot of wave number `(barv)` against`((1)/(n^(2)))` will be (The Rydberg constant, `R_(H)` is in wave number unit)

A

Linear with slope `-R_(H)`

B

Non linear

C

Linear with slope `R_(H)`

D

Linear with intercept

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To solve the problem, we need to analyze the emission lines of atomic hydrogen as it transitions from an initial energy level \( n_i = 8 \) to a final energy level \( n_f = n \). We will derive the relationship between the wave number \( \bar{v} \) and \( \frac{1}{n^2} \). ### Step 1: Understand the formula for wave number The wave number \( \bar{v} \) is related to the Rydberg formula for hydrogen: \[ \bar{v} = R_H \left( \frac{1}{n_i^2} - \frac{1}{n_f^2} \right) \] where \( R_H \) is the Rydberg constant. ### Step 2: Substitute the initial and final states Given that \( n_i = 8 \) and \( n_f = n \), we can substitute these values into the formula: \[ \bar{v} = R_H \left( \frac{1}{8^2} - \frac{1}{n^2} \right) \] Calculating \( 8^2 \): \[ 8^2 = 64 \] Thus, we have: \[ \bar{v} = R_H \left( \frac{1}{64} - \frac{1}{n^2} \right) \] ### Step 3: Rearranging the equation We can express this equation in terms of \( \frac{1}{n^2} \): \[ \bar{v} = R_H \left( \frac{1}{64} \right) - R_H \left( \frac{1}{n^2} \right) \] This can be rewritten as: \[ \bar{v} = -R_H \left( \frac{1}{n^2} \right) + R_H \left( \frac{1}{64} \right) \] ### Step 4: Identify the linear relationship This equation is in the form of \( y = mx + c \), where: - \( y \) is \( \bar{v} \) - \( m \) (the slope) is \( -R_H \) - \( x \) is \( \frac{1}{n^2} \) - \( c \) (the y-intercept) is \( R_H \left( \frac{1}{64} \right) \) ### Step 5: Conclusion about the plot Since the relationship between \( \bar{v} \) and \( \frac{1}{n^2} \) is linear, we conclude that the plot of wave number \( \bar{v} \) against \( \frac{1}{n^2} \) will be a straight line with a negative slope. ### Final Answer The plot of wave number \( \bar{v} \) against \( \frac{1}{n^2} \) will be linear with a negative slope. ---

To solve the problem, we need to analyze the emission lines of atomic hydrogen as it transitions from an initial energy level \( n_i = 8 \) to a final energy level \( n_f = n \). We will derive the relationship between the wave number \( \bar{v} \) and \( \frac{1}{n^2} \). ### Step 1: Understand the formula for wave number The wave number \( \bar{v} \) is related to the Rydberg formula for hydrogen: \[ \bar{v} = R_H \left( \frac{1}{n_i^2} - \frac{1}{n_f^2} \right) \] where \( R_H \) is the Rydberg constant. ...
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