The value of \( \frac{1}{r} \) in the \( \psi_{1,0,0}(r,\theta,\phi) \) state of a hydrogen atom is:
\[ \psi_{1,0,0}(r,\theta,\phi) = \frac{1}{\sqrt{\pi a_0^3}} e^{-r/a_0} \] In this equation, the wave function \( \psi_{1,0,0}(r,\theta,\phi) \) describes the ground state (1s state) of the hydrogen atom. The Bohr radius \( a_0 \) is a fundamental constant and represents the most probable distance of the electron from the nucleus in the ground state.
Correct Answer:
\( \frac{1}{a_0} \)
To solve for \( \frac{1}{r} \), observe the exponential form of the wave function. The term \( e^{-r/a_0} \) represents a decaying function with respect to \( r \), and this function will approach 0 as \( r \) becomes very large. The Bohr radius \( a_0 \) is the scale factor that defines the characteristic size of the hydrogen atom. Therefore, the inverse of the radial coordinate \( r \) in this state is given by \( \frac{1}{a_0} \), which is consistent with the ground state of the hydrogen atom.
List I (Spectral Lines of Hydrogen for transitions from) | List II (Wavelength (nm)) | ||
A. | n2 = 3 to n1 = 2 | I. | 410.2 |
B. | n2 = 4 to n1 = 2 | II. | 434.1 |
C. | n2 = 5 to n1 = 2 | III. | 656.3 |
D. | n2 = 6 to n1 = 2 | IV. | 486.1 |
The angular momentum of an electron in a stationary state of \(Li^{2+}\) (\(Z=3\)) is \( \frac{3h}{\pi} \). The radius and energy of that stationary state are respectively.