For He + ion, the wave number associated with the Balmer transition, n = 4 to n = 2 is given by :
v- = \(\frac{1}{\lambda}\) = RZ2 (\(\frac{1}{n_1^2}-\frac{1}{n_2^2}\))
Where, n1 = 2 ,n2 = 4 , Z = atomic number of helium
v- = \(\frac{1}{\lambda}\) = R (2)2 (\(\frac{1}{4}-\frac{1}{6}\)) = 4R (\(\frac{4-1}{16}\))
v- = \(\frac{1}{\lambda}\) = \(\frac{3R}{4}\) ⇒ λ = \(\frac{4}{3R}\)
According to the question, the desired transition for hydrogen will have the same wavelength as that of He+.
⇒ R(1)2[\(\frac{1}{n_1^2}-\frac{1}{n_2^2}\)] = \(\frac{3R}{4}\)
By hit and trail method, the equality given by equation (1) is true only when n1 = 1 and n2 = 2.
∴ The transition for n2 = 2 to n = 1 in the hydrogen spectrum would have the same wavelength as the Balmer transition n = 4 to n= 2 of He+ spectrum.
Considering Bohr’s atomic model for hydrogen atom :
(A) the energy of H atom in ground state is same as energy of He+ ion in its first excited state.
(B) the energy of H atom in ground state is same as that for Li++ ion in its second excited state.
(C) the energy of H atom in its ground state is same as that of He+ ion for its ground state.
(D) the energy of He+ ion in its first excited state is same as that for Li++ ion in its ground state.
Draw the Lewis structures for the following molecules and ions: \(H_2S\), \(SiCl_4\), \(BeF_2\), \(CO_3^{2-}\) , \(HCOOH\)
The atomic structure of an element refers to the constitution of its nucleus and the arrangement of the electrons around it. Primarily, the atomic structure of matter is made up of protons, electrons and neutrons.
Dalton proposed that every matter is composed of atoms that are indivisible and indestructible.
The following are the postulates of his theory:
Several atomic structures of an element can exist, which differ in the total number of nucleons.These variants of elements having a different nucleon number (also known as the mass number) are called isotopes of the element. Therefore, the isotopes of an element have the same number of protons but differ in the number of neutrons. For example, there exist three known naturally occurring isotopes of hydrogen, namely, protium, deuterium, and tritium.