Step 1: Bohr's Quantization Condition
Bohr's condition states that the angular momentum of an electron in the \(n^{th}\) orbit is quantized: \( L = mvr = n \frac{h}{2\pi} \). Here, \(m\) is the electron's mass, \(v\) its velocity, \(r\) the orbital radius, and \(h\) is Planck's constant.
Step 2: de Broglie Wavelength
The de Broglie wavelength (\( \lambda \)) of an electron is given by \( \lambda = \frac{h}{p} = \frac{h}{mv} \), where \(p\) is momentum. Substituting \( mv = \frac{nh}{2\pi r} \) from Bohr's condition yields \( \lambda = \frac{h}{\frac{nh}{2\pi r}} = \frac{2\pi r}{n} \).
Step 3: For \(n = 2\)
For the \(n = 2\) state, the wavelength is \( \lambda = \frac{2\pi r_2}{2} = \pi r_2 \). The radius of the \(n^{th}\) Bohr orbit is \( r_n = n^2 a_0 \), with \(a_0\) being the Bohr radius (0.052 nm). For \(n = 2\), \( r_2 = 2^2 a_0 = 4 \times 0.052 \text{ nm} = 0.208 \text{ nm} \).
Step 4: Calculate the de Broglie Wavelength
The de Broglie wavelength for \(n = 2\) is calculated as \( \lambda = \pi r_2 = \pi \times 0.208 \text{ nm} \approx 3.14 \times 0.208 \text{ nm} \approx 0.653 \text{ nm} \).
Conclusion
A discrepancy exists with the provided options; however, 0.67 nm is the closest value to 0.653 nm.