| λ (nm) | 500 | 450 | 400 |
|---|---|---|---|
| v × 10–5(cm s–1) | 2.55 | 4.35 | 5.35 |
(a) Assuming the threshold wavelength to be λ0 nm (= λ0 × 10-9 m) , the kinetic energy of the radiation is given as: h (v - v0) = \(\frac{1}{2}\)mv2
Three different equalities can be formed by the given value as:
hc (\(\frac{1}{\lambda}-\frac{1}{\lambda_0}\)) =\(\frac{1}{2}\)mv2
hc (\(\frac{1}{500\times10^{9}}-\frac{1}{\lambda_0\times10^{-9}m}\)) = \(\frac{1}{2}\)m (2.55 × 10+5 × 10-2 ms-1)
\(\frac{hc}{10^{-9}}m[\frac{1}{500}-\frac{1}{\lambda_0}]=\frac{1}{2}m\)(2.55 × 10+3 ms-1)2 …....(1)
Similarly,\(\frac{hc}{10^{-9}m}\) [\(\frac{1}{450}-\frac{1}{\lambda_0}\)] = \(\frac{1}{2}m\) (3.45 × 10+3 ms-1)2 …...(2)
\(\frac{hc}{10^{-9}m}\)[\(\frac{1}{400}-\frac{1}{\lambda_0}\)] = \(\frac{1}{2}\) m (5.35×10+3 ms-1)2 …....(3)
Dividing equation (3) by equation (1):
\(\frac{[\frac{\lambda_0-400}{400\lambda_0}]}{[\frac{\lambda_0-500}{500\lambda_0}]}=\frac{(5.35\times10^{+3}ms^{-1})^2}{(2.55\times10^{+3}ms^{-1})^2}\)
\(\frac{5\lambda_0-2000}{4\lambda_0-2000}=(\frac{5.35}{2.55})^2=\frac{28.6225}{6.5025}\)
\(\frac{5\lambda_0-2000}{4\lambda_0-2000}=4.40177\)
17.6070 λ0 - 5 λ0 = 8803.537 - 2000
λ0 = \(\frac{ 680.537}{12.607}\)
λ0 = 539.8 nm
λ0 ≈ 540 nm
∴ Threshold wavelength (λ0) = 540 nm
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.
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.