The radius of the nth Bohr orbit for a hydrogen-like species is given by:
\( r = \frac{n^2a_0}{Z} \)
where n is the principal quantum number, \(a_0\) is the Bohr radius for hydrogen, and Z is the atomic number. For the 1st Bohr orbit of hydrogen (n = 1, Z = 1), \(r = a_0\).
We need to find a species where \(r = a_0\). Let us check the options:
\( r = \frac{2^2a_0}{3} = \frac{4}{3}a_0 \)
\( r = \frac{2^2a_0}{4} = a_0 \)
\( r = \frac{2^2a_0}{2} = 2a_0 \)
\( r = \frac{3^2a_0}{3} = 3a_0 \)
Only option 2 gives the same radius as the 1st Bohr orbit of hydrogen.
A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: