Need of Quantum Theory ( Black body radiation )

Introductory Wave Mechanics

Need of Quantum Theory ( Black body radiation )

Important equaiton to be remember:

  • $$u(\nu, T)= \frac{8\pi\nu^2}{c^3}\times$$
  • <...}

Inadequacies of classical Mechanics

Introductory Wave Mechanics

Inadequacies of classical Mechanics

Inadequacies of classical Mechanics:

  1.  It could not explain the spectr...}

Wave-Matter duality of radiation

Introductory Wave Mechanics

Wave-Matter duality of radiation

  • According to Plank's theory of radiation energy of photon of frequency \(\nu\) is given...}

de-Broglie Wavelength of relativistic particle

Introductory Wave Mechanics

de-Broglie Wavelength of relativistic particle

  • The de-Broglie wavelength of particle is given by,

    $$\lambda=\frac{h}{p}$$

    <...}

Calculation of de-Broglie wavelength of neutrino, diatomic gas and poly-atomic gas

Introductory Wave Mechanics

Calculation of de-Broglie wavelength of neutrino, diatomic gas and poly-atomic gas

  1. de-Broglie wavelength of poly-atomic gas $$=\frac{h}{\sqrt{2mKT}}$$
  2. de-Brogli...}

Phase velocity and group velocity

Introductory Wave Mechanics

Phase velocity and group velocity

  1. The velocity of a complete wave profile is known as phase velocity or it is also defined as...}

Derivation for Group velocity

Introductory Wave Mechanics

Derivation for Group velocity

  • $$= A sin\biggl[\biggl(k+\frac{\Delta k}{2}\biggr)x-\biggl(\omega+\frac{\Delta \omega}{...}

Relation between group velocity and particle velocity

Introductory Wave Mechanics

Relation between group velocity and particle velocity

  • \(\Delta x\cdot \Delta P_x= h<\frac{hbar}{2}\) from the concept of wave packet.

    ...}

Superposition of plane waves

Introductory Wave Mechanics

Superposition of plane waves

  • $$\psi (x,t)= \sum_{i=1}^\infty A_i e^{i(k_i x- \omega_i t)}\dotsm(1)$$
  •  ...}

Particles wave packet spreads in time

Introductory Wave Mechanics

Particles wave packet spreads in time

  • $$\psi(x,t)= \int_{-\infty}^\infty e^{-\sigma(k-k_0)^2} e^{i(kx-\omega(k_0)t-(k-k_0)tv_...}