λp > λα > λe
λα > λp > λe
λe > λp > λα
λe > λα > λp
\(\lambda _{e}=\frac{h}{\sqrt{\frac{2\times m}{2000}}\times4K}=\frac{10\sqrt{20h}}{2\sqrt{2mK}}\)
\(\lambda _{p}=\frac{h}{\sqrt{2mK}}=\frac{h}{\sqrt{2mK}}\)
\(\lambda _{\alpha }=\frac{h}{\sqrt{2\times 4m\times 2K}}=\frac{h}{4\sqrt{mK}}\)
\(\lambda _{e}>\lambda _{p}>\lambda _{\alpha }\)
So, the correct option is (C): λe > λp > λα
The De Broglie wavelength of a particle is given by the equation:
λ = \(\frac{h}{p}\)
where λ is the wavelength, h is the Planck constant, and p is the momentum of the particle.
Since the kinetic energy of the particles is given, we can use the relation:
K = \(\frac{p^2}{2m}\)
where K is the kinetic energy, p is the momentum, and m is the mass of the particle.
Solving for momentum, we get:
p = \(\sqrt{(2mK)}\)
Using this expression for each particle and substituting in the equation for De Broglie wavelength, we get:
\(\lambda_e=\frac{h}{\sqrt{(2mK)}}\)
\(\lambda_p=\frac{h}{\sqrt{(4mK)}}\) = \(\frac{h}{\sqrt{(2m)}\sqrt{(2K)}}\)
\(\lambda_\alpha=\frac{h}{\sqrt{(4\alpha mK)}}\)
where α is the ratio of the mass of the alpha particle to the mass of the hydrogen atom.
Since the mass of the proton is approximately the same as the mass of the hydrogen atom, we can write:
α = \(\frac{m\alpha}{mH}=\frac{4}{1}\) = 4
Therefore, we have:
\(\lambda_e=\frac{h}{\sqrt{(2mK)}}\)
\(\lambda_p=\frac{h}{\sqrt{(2m)}\sqrt{(2k)}}\)
\(\lambda_\alpha=\frac{h}{\sqrt{(16mK)}}\)
Simplifying these expressions, we get:
\(\lambda_e=\frac{h}{\sqrt{(2mK)}}\)
\(\lambda_p=\frac{h}{\sqrt{(4mK)}}\)
\(\lambda_\alpha=\frac{h}{4\sqrt{mK}}\)
Since \(\sqrt{(2mK)}>\sqrt{(4mK)}>\frac{1}{(4\sqrt{mK})}\),
We can conclude that: λe > λp > λα
Therefore, the correct option is (C).
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.