If the potential energy of a hydrogen atom in the first excited state (\(n = 2\)) is assumed to be zero, then we must adjust the energy reference accordingly.
Normally, for hydrogen:
If we set \(U_2 = 0\), the energy levels shift by \(+6.8\, \text{eV}\).
Now, at \(n = \infty\), total energy in the usual reference is:
\[ E_\infty = 0 \] After the shift: \[ E_\infty' = 0 + 6.8 - 3.4 = \boxed{3.4\, \text{eV}} \]
Correct answer: 3.4 eV
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
A hydrogen-like atom consists of a tiny positively-charged nucleus and an electron revolving around the nucleus in a stable circular orbit.
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.
The Bohr Model was an important step in the development of atomic theory. However, it has several limitations.