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ElectricalElectrical Materials
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The quantized value of energy is given by

A

E=h28mL2(nx2+ny2+nz2)E = \frac{h^2}{8mL^2}(n_x^2 + n_y^2 + n_z^2)E=8mL2h2тАЛ(nx2тАЛ+ny2тАЛ+nz2тАЛ)

B

n=(nx2+ny2+nz2)n = (n_x^2 + n_y^2 + n_z^2)n=(nx2тАЛ+ny2тАЛ+nz2тАЛ)

C

n=18├Ч4╧А3n3n = \frac{1}{8} \times \frac{4\pi}{3} n^3n=81тАЛ├Ч34╧АтАЛn3

D

None

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalElectrical Materials
Option A

E=h28mL2(nx2+ny2+nz2)E = \frac{h^2}{8mL^2}(n_x^2 + n_y^2 + n_z^2)E=8mL2h2тАЛ(nx2тАЛ+ny2тАЛ+nz2тАЛ)

Quick Summary:

The quantized energy of a particle of mass 'm' trapped in a three-dimensional infinite potential well (box) of side length 'L' is given by the expression derived from solving the Schr├╢dinger equation. This model illustrates the confinement of particles, where energy levels are restricted to discrete values based on quantum numbers nx,ny,n_x, n_y,nxтАЛ,nyтАЛ, and nzn_znzтАЛ.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The quantized energy of a particle of mass 'm' trapped in a three-dimensional infinite potential well (box) of side length 'L' is given by the expression derived from solving the Schr├╢dinger equation. This model illustrates the confinement of particles, where energy levels are restricted to discrete values based on quantum numbers nx,ny,n_x, n_y,nxтАЛ,nyтАЛ, and nzn_znzтАЛ.

ЁЯФв Key Formulas

E=h28mL2(nx2+ny2+nz2)E = \frac{h^2}{8mL^2}(n_x^2 + n_y^2 + n_z^2)E=8mL2h2тАЛ(nx2тАЛ+ny2тАЛ+nz2тАЛ) тАФ Quantized energy for a 3D potential well

╬и(x,y,z)=8VsinтБб(nx╧АxL)sinтБб(ny╧АyL)sinтБб(nz╧АzL)\Psi(x,y,z) = \sqrt{\frac{8}{V}} \sin(\frac{n_x \pi x}{L}) \sin(\frac{n_y \pi y}{L}) \sin(\frac{n_z \pi z}{L})╬и(x,y,z)=V8тАЛтАЛsin(LnxтАЛ╧АxтАЛ)sin(LnyтАЛ╧АyтАЛ)sin(LnzтАЛ╧АzтАЛ) тАФ Normalized wave function

тЪЩя╕П Working Principle

For a 3D box, the wave function must vanish at the boundaries (x,y,z=0,Lx,y,z = 0, Lx,y,z=0,L). This boundary condition leads to quantized wave vectors kx=nx╧АLk_x = \frac{n_x \pi}{L}kxтАЛ=LnxтАЛ╧АтАЛ, ky=ny╧АLk_y = \frac{n_y \pi}{L}kyтАЛ=LnyтАЛ╧АтАЛ, and kz=nz╧АLk_z = \frac{n_z \pi}{L}kzтАЛ=LnzтАЛ╧АтАЛ. Substituting these into the energy equation E=тДП2k22mE = \frac{\hbar^2 k^2}{2m}E=2mтДП2k2тАЛ, where k2=kx2+ky2+kz2k^2 = k_x^2 + k_y^2 + k_z^2k2=kx2тАЛ+ky2тАЛ+kz2тАЛ and тДП=h2╧А\hbar = \frac{h}{2\pi}тДП=2╧АhтАЛ, we arrive at the energy expression E=h28mL2(nx2+ny2+nz2)E = \frac{h^2}{8mL^2}(n_x^2 + n_y^2 + n_z^2)E=8mL2h2тАЛ(nx2тАЛ+ny2тАЛ+nz2тАЛ).

ЁЯУМ Key Points
  • тЦ╕

    The energy levels depend on three independent quantum numbers.

  • тЦ╕

    The ground state energy occurs when nx=ny=nz=1n_x=n_y=n_z=1nxтАЛ=nyтАЛ=nzтАЛ=1.

  • тЦ╕

    Energy increases as the volume V=L3V = L^3V=L3 of the box decreases.

  • тЦ╕

    This model serves as the foundational concept for the electron gas theory in metals.

тЬЕ Advantages
  • тЦ╕

    Predicts discrete energy spectra for confined electrons.

  • тЦ╕

    Explains phenomena like quantum dots and size-dependent bandgaps.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Assumes an infinite potential barrier, which is an idealization.

  • тЦ╕

    Ignores electron-electron interactions.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Quantum Dots and Nanoparticles

  • тЦ╕

    Semiconductor physics

  • тЦ╕

    Statistical mechanics of ideal gases

ЁЯУД Additional Information
  • тЦ╕

    For a 1D box, the expression simplifies to E=n2h28mL2E = \frac{n^2 h^2}{8mL^2}E=8mL2n2h2тАЛ.

  • тЦ╕

    Option B is incorrect because it relates only to indices, not energy.

  • тЦ╕

    Option C represents the volume calculation in k-space used to derive the density of states.

ЁЯУК Diagram / Illustration
Energy Quantization in 3D BoxE = (h┬▓ / 8mL┬▓) ├Ч (nтВУ┬▓ + n_y┬▓ + n_z┬▓)Where nтВУ, n_y, n_z = 1, 2, 3, ...
тЬЕ

A is correct тАФ The formula represents the discrete energy eigenvalues of a particle confined in a three-dimensional cubic potential well of length L.

Core Concepts Used
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Quantum Confinement Schr├╢dinger Equation Infinite Potential Well
ЁЯТб EXAM TIP

Always remember that in quantum confinement, as the physical dimensions (L) shrink, the energy level spacing increases, which is why nanoparticles show different colors compared to bulk materials.

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