Radius of the first orbit in H-atom is \(a_0\). Then, de Broglie wavelength of electron in the third orbit is.
3\(\pi\)a0
6\(\pi\)a0
9\(\pi\)a0
12\(\pi\)a0
To determine the de Broglie wavelength of the electron in the third orbit of the hydrogen atom, we begin by using de Broglie's hypothesis, which states that an electron orbiting a nucleus could be treated as a wave, with its wavelength given by:
\(\lambda = \frac{h}{mv}\)
For an electron in a circular orbit, de Broglie's hypothesis leads to the condition for stable orbit, which is:
\(n\lambda = 2\pi r_n\)
where \( n \) is the principal quantum number and \( r_n \) is the radius of the \( n \)-th orbit.
From Bohr's model, the radius of the \( n \)-th orbit (\( r_n \)) is given by:
\(r_n = n^2 a_0\)
For the third orbit (\( n = 3 \)),
\(r_3 = 3^2 a_0 = 9 a_0\)
Substituting back into the condition for stable orbit, we get:
\(3\lambda = 2\pi \times 9a_0\)
Simplifying, we find the wavelength:
\(\lambda = \frac{2\pi \times 9a_0}{3} = 6\pi a_0\)
Thus, the de Broglie wavelength of the electron in the third orbit is 6\(\pi\)a0.