307545
The wave function \((\Psi)\) of 2 s is given by \({\Psi _{2{\rm{s}}}} = \frac{1}{{2\sqrt {2\pi } }}{\left( {\frac{1}{{{{\rm{a}}_{\rm{0}}}}}} \right)^{1/2}}\left( {2 - \frac{{\rm{r}}}{{{{\rm{a}}_{\rm{0}}}}}} \right){{\rm{e}}^{ - {\rm{r}}/2{{\rm{a}}_0}}}\)
At \({\rm{r}} = {{\rm{r}}_{\rm{0}}}\), radial node is formed. Thus, \(r_{0}\) in terms of \(\mathrm{a}_{0}\)
307546
Electron of \(\mathrm{Be}^{3+}\) ion is present in an orbital which has 2 angular nodes and 2 radial nodes. Calculate sum of \(({\rm{n}} + l)\) for orbital in which electron is present.
(Given: In this question, n is principal quantum number and l is azimuthal quantum number).
307545
The wave function \((\Psi)\) of 2 s is given by \({\Psi _{2{\rm{s}}}} = \frac{1}{{2\sqrt {2\pi } }}{\left( {\frac{1}{{{{\rm{a}}_{\rm{0}}}}}} \right)^{1/2}}\left( {2 - \frac{{\rm{r}}}{{{{\rm{a}}_{\rm{0}}}}}} \right){{\rm{e}}^{ - {\rm{r}}/2{{\rm{a}}_0}}}\)
At \({\rm{r}} = {{\rm{r}}_{\rm{0}}}\), radial node is formed. Thus, \(r_{0}\) in terms of \(\mathrm{a}_{0}\)
307546
Electron of \(\mathrm{Be}^{3+}\) ion is present in an orbital which has 2 angular nodes and 2 radial nodes. Calculate sum of \(({\rm{n}} + l)\) for orbital in which electron is present.
(Given: In this question, n is principal quantum number and l is azimuthal quantum number).
307545
The wave function \((\Psi)\) of 2 s is given by \({\Psi _{2{\rm{s}}}} = \frac{1}{{2\sqrt {2\pi } }}{\left( {\frac{1}{{{{\rm{a}}_{\rm{0}}}}}} \right)^{1/2}}\left( {2 - \frac{{\rm{r}}}{{{{\rm{a}}_{\rm{0}}}}}} \right){{\rm{e}}^{ - {\rm{r}}/2{{\rm{a}}_0}}}\)
At \({\rm{r}} = {{\rm{r}}_{\rm{0}}}\), radial node is formed. Thus, \(r_{0}\) in terms of \(\mathrm{a}_{0}\)
307546
Electron of \(\mathrm{Be}^{3+}\) ion is present in an orbital which has 2 angular nodes and 2 radial nodes. Calculate sum of \(({\rm{n}} + l)\) for orbital in which electron is present.
(Given: In this question, n is principal quantum number and l is azimuthal quantum number).
307545
The wave function \((\Psi)\) of 2 s is given by \({\Psi _{2{\rm{s}}}} = \frac{1}{{2\sqrt {2\pi } }}{\left( {\frac{1}{{{{\rm{a}}_{\rm{0}}}}}} \right)^{1/2}}\left( {2 - \frac{{\rm{r}}}{{{{\rm{a}}_{\rm{0}}}}}} \right){{\rm{e}}^{ - {\rm{r}}/2{{\rm{a}}_0}}}\)
At \({\rm{r}} = {{\rm{r}}_{\rm{0}}}\), radial node is formed. Thus, \(r_{0}\) in terms of \(\mathrm{a}_{0}\)
307546
Electron of \(\mathrm{Be}^{3+}\) ion is present in an orbital which has 2 angular nodes and 2 radial nodes. Calculate sum of \(({\rm{n}} + l)\) for orbital in which electron is present.
(Given: In this question, n is principal quantum number and l is azimuthal quantum number).