Some energy levels of a molecule are shown in the picture, the proportion of wavelength will be the value of
(a) r = 4/3. (b) r = 2/3
(c) r = 3/4. (d) r = 1/3
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21
We know,
hc/lamda = delta(E)
In this diagram,
The electron looses energy and jumps from higher energy level to lower,
Therefore the electron has a better all round stability and we observe wavelength of different lamda on different jumps of electron.
Where,
delta(E) = change in energy
Now ATQ,
For the first wavelength,
Lamda(1) = hc/delta(E)
= hc/{-E-(-2E)}
= hc/E....(1)
For second wavelength,
Lamda(2) = hc/delta(E)
= hc/{-E-(-4E/3)}
= 3hc/E.... (2)
From (1) and (2),
Taking ratios of both the wavelength,
Lamda(1)/lamda(2) = 1/3
So, the correct option is (d).
hc/lamda = delta(E)
In this diagram,
The electron looses energy and jumps from higher energy level to lower,
Therefore the electron has a better all round stability and we observe wavelength of different lamda on different jumps of electron.
Where,
delta(E) = change in energy
Now ATQ,
For the first wavelength,
Lamda(1) = hc/delta(E)
= hc/{-E-(-2E)}
= hc/E....(1)
For second wavelength,
Lamda(2) = hc/delta(E)
= hc/{-E-(-4E/3)}
= 3hc/E.... (2)
From (1) and (2),
Taking ratios of both the wavelength,
Lamda(1)/lamda(2) = 1/3
So, the correct option is (d).
Answered by
0
As we learnt in
Energy emitted due to transition of electron -
\Delta E= Rhcz^{2}\left ( \frac{1}{n_{f}\, ^{2}}-\frac{1}{n_{i}\, ^{2}} \right )
\frac{1}{\lambda }= Rz^{2}\left ( \frac{-1}{n_{i}\, ^{2}}+\frac{1}{n_{f}\, ^{2}} \right )
- wherein
R= R hydberg\: constant
n_{i}= initial state \\n_{f}= final \: state
From the figure.
\lambda_{1}=\frac{hc}{\Delta E_{1}}=\frac{hc}{-E-(-2t)}=\frac{hc}{E}
\lambda_{2}=\frac{hc}{-E-\left(-\frac{4E}{3} \right )}-\frac{hc}{(\frac{E}{3})}.3\frac{hc}{E}
\frac{\lambda_1}{\lambda_2}=\frac{1}{3}
Correct option is 4
Option 1)
r= \frac{4}{3}
This is an incorrect option.
Option 2)
r= \frac{2}{3}
This is an incorrect option.
Option 3)
r= \frac{3}{4}
This is an incorrect option.
Option 4)
This is the correct option.
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