If electrons did not have intrinsic angular momentum (spin) but still obeyed the Pauli exclusion principle the states occupied by electrons in the ground state of helium would be:
A) (n = 1,

); (n = 1, If electrons did not have intrinsic angular momentum (spin) but still obeyed the Pauli exclusion principle the states occupied by electrons in the ground state of helium would be: A) (n = 1, ); (n = 1, ) B) (n = 1, ); (n = 1, ) C) (n = 1, ); (n = 2, ) D) (n = 2, ); (n = 2, ) E) (n = 2, ); (n = 2, )

)
B) (n = 1, If electrons did not have intrinsic angular momentum (spin) but still obeyed the Pauli exclusion principle the states occupied by electrons in the ground state of helium would be: A) (n = 1, ); (n = 1, ) B) (n = 1, ); (n = 1, ) C) (n = 1, ); (n = 2, ) D) (n = 2, ); (n = 2, ) E) (n = 2, ); (n = 2, )

)
C) (n = 1, If electrons did not have intrinsic angular momentum (spin) but still obeyed the Pauli exclusion principle the states occupied by electrons in the ground state of helium would be: A) (n = 1, ); (n = 1, ) B) (n = 1, ); (n = 1, ) C) (n = 1, ); (n = 2, ) D) (n = 2, ); (n = 2, ) E) (n = 2, ); (n = 2, )

); (n = 2, If electrons did not have intrinsic angular momentum (spin) but still obeyed the Pauli exclusion principle the states occupied by electrons in the ground state of helium would be: A) (n = 1, ); (n = 1, ) B) (n = 1, ); (n = 1, ) C) (n = 1, ); (n = 2, ) D) (n = 2, ); (n = 2, ) E) (n = 2, ); (n = 2, )

)
D) (n = 2, If electrons did not have intrinsic angular momentum (spin) but still obeyed the Pauli exclusion principle the states occupied by electrons in the ground state of helium would be: A) (n = 1, ); (n = 1, ) B) (n = 1, ); (n = 1, ) C) (n = 1, ); (n = 2, ) D) (n = 2, ); (n = 2, ) E) (n = 2, ); (n = 2, )

)
E) (n = 2, If electrons did not have intrinsic angular momentum (spin) but still obeyed the Pauli exclusion principle the states occupied by electrons in the ground state of helium would be: A) (n = 1, ); (n = 1, ) B) (n = 1, ); (n = 1, ) C) (n = 1, ); (n = 2, ) D) (n = 2, ); (n = 2, ) E) (n = 2, ); (n = 2, )

)

Possible Values of the Principal Quantum Number N for an Electron

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