Question:

For the hydrogen spectrum,the wavelength in Balmer series is given by \(\frac{1}{λ}\)=R(\(\frac{1}{n_{1}^{2}}\)-\(\frac{1}{n_{2}^{2}}\)) where λ= wavelength and R is Rydberg constant. What are the values of n1 and n2,for the longest wavelength in the Balmer series?

Updated On: Apr 7, 2025
  • n1=2,n2=3 

  • n1=2,n2=4

  • n1=1,n2=2 

  • n1=2,n2=∞

  • n1=3,n2=∞

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The Correct Option is A

Approach Solution - 1

Given:

  • Balmer series formula for hydrogen spectrum: \[ \frac{1}{\lambda} = R \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \]
  • We need to find \( n_1 \) and \( n_2 \) for the longest wavelength in the Balmer series.

Step 1: Understand the Balmer Series

The Balmer series corresponds to transitions where the electron falls to the \( n_1 = 2 \) level. Thus, \( n_1 \) is fixed as 2.

Step 2: Determine \( n_2 \) for Longest Wavelength

The longest wavelength occurs when the energy difference is smallest, i.e., for the smallest possible transition:

\[ n_2 = n_1 + 1 = 3 \]

Substituting \( n_1 = 2 \) and \( n_2 = 3 \):

\[ \frac{1}{\lambda} = R \left( \frac{1}{2^2} - \frac{1}{3^2} \right) = R \left( \frac{1}{4} - \frac{1}{9} \right) = R \left( \frac{5}{36} \right) \]

This gives the smallest \( \frac{1}{\lambda} \), and thus the largest \( \lambda \).

Conclusion:

The values of \( n_1 \) and \( n_2 \) for the longest wavelength in the Balmer series are \( n_1 = 2 \) and \( n_2 = 3 \).

Answer: \(\boxed{A}\)

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Approach Solution -2

Step 1: Recall the Balmer series formula and conditions for the longest wavelength.

The Balmer series corresponds to transitions of electrons in hydrogen atoms where the final energy level is \( n_1 = 2 \). The formula for the reciprocal of the wavelength is:

\[ \frac{1}{\lambda} = R \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right), \]

where:

  • \( \lambda \) is the wavelength,
  • \( R \) is the Rydberg constant,
  • \( n_1 = 2 \) (for the Balmer series), and
  • \( n_2 > n_1 \) (the initial energy level).

The wavelength is inversely proportional to \( \frac{1}{\lambda} \). For the longest wavelength, \( \frac{1}{\lambda} \) must be minimized. This occurs when \( n_2 \) is the smallest integer greater than \( n_1 \), i.e., \( n_2 = 3 \).

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Step 2: Identify the values of \( n_1 \) and \( n_2 \).

For the Balmer series:

  • \( n_1 = 2 \) (fixed for the Balmer series),
  • \( n_2 = 3 \) (smallest value greater than \( n_1 \) to minimize \( \frac{1}{\lambda} \)).

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Final Answer: The values of \( n_1 \) and \( n_2 \) for the longest wavelength in the Balmer series are \( \mathbf{n_1 = 2, n_2 = 3} \), which corresponds to option \( \mathbf{(A)} \).

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Concepts Used:

Bohr's Model of Hydrogen Atom

Niels Bohr introduced the atomic Hydrogen model in 1913. He described it as a positively charged nucleus, comprised of protons and neutrons, surrounded by a negatively charged electron cloud. In the model, electrons orbit the nucleus in atomic shells. The atom is held together by electrostatic forces between the positive nucleus and negative surroundings.

Read More: Bohr's Model of Hydrogen Atom

Bohr's Theory of Hydrogen Atom and Hydrogen-like Atoms

A hydrogen-like atom consists of a tiny positively-charged nucleus and an electron revolving around the nucleus in a stable circular orbit. 

Bohr's Radius: 

If 'e,' 'm,' and 'v' be the charge, mass, and velocity of the electron respectively, 'r' be the radius of the orbit, and Z be the atomic number, the equation for the radii of the permitted orbits is given by r = n2 xr1, where 'n' is the principal quantum number, and r1 is the least allowed radius for a hydrogen atom, known as Bohr's radius having a value of 0.53 Å. 

Limitations of the Bohr Model

The Bohr Model was an important step in the development of atomic theory. However, it has several limitations.

  1. Bohr’s model of the atom failed to explain the Zeeman Effect (effect of magnetic field on the spectra of atoms).
  2. It failed to explain the Stark effect (effect of electric field on the spectra of atoms).
  3. The spectra obtained from larger atoms weren’t explained.
  4. It violates the Heisenberg Uncertainty Principle.