To solve the problem, we need to determine the radius of the third Bohr orbit of the Li2+ ion. Let's start with the known formula for the radius of the nth Bohr orbit: \(r_n = \frac {n^2 × a_0}{Z}\),
where a0 is the Bohr radius (approximately 52.9 pm), n is the principal quantum number, and Z is the atomic number of the ion.
Given:
Formula for radius:
For He+, \(r_n = \frac {n^2 × a_0}{Z}\)
\(105.8 = \frac {2^2 × a_0}{2}\)
\(105.8 = 2 × a_0\)
Solving for a0:
Now, calculate the radius for the third Bohr orbit of Li2+:
Formula: \(r_n = \frac {n^2 × a_0}{Z}\)
\(r_3 = \frac {(3^2) × 52.9}{3}\)
\(r_3 =\frac{ (9) × 52.9}{3}\)
\(r_3 = 158.7\) pm
Thus, the radius of the third Bohr orbit of Li2+ ion is 158.7 pm.
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
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.