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Chapter 1 of 12 • Page 1 of 248🔒 Protected PDF • Watermarked
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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=8mL2h2​(nx2​+ny2​+nz2​)

B

n=(nx2+ny2+nz2)n = (n_x^2 + n_y^2 + n_z^2)n=(nx2​+ny2​+nz2​)

C

n=18×4π3n3n = \frac{1}{8} \times \frac{4\pi}{3} n^3n=81​×34π​n3

D

None

Correct Answer

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=8mL2h2​(nx2​+ny2​+nz2​)

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 Schrödinger equation. This model illustrates the confinement of particles, where energy levels are restricted to discrete values based on quantum numbers $n_x, n_y,$ and $n_z$.

💡 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 Schrödinger 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,nx​,ny​, and nzn_znz​.

🔢 Key Formulas

E=h28mL2(nx2+ny2+nz2)E = \frac{h^2}{8mL^2}(n_x^2 + n_y^2 + n_z^2)E=8mL2h2​(nx2​+ny2​+nz2​) — Quantized energy for a 3D potential well

Ψ(x,y,z)=8Vsin⁡(nxπxL)sin⁡(nyπyL)sin⁡(nzπzL)\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})Ψ(x,y,z)=V8​​sin(Lnx​πx​)sin(Lny​πy​)sin(Lnz​πz​) — Normalized wave function

⚙️ 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=nxπLk_x = \frac{n_x \pi}{L}kx​=Lnx​π​, ky=nyπLk_y = \frac{n_y \pi}{L}ky​=Lny​π​, and kz=nzπLk_z = \frac{n_z \pi}{L}kz​=Lnz​π​. Substituting these into the energy equation E=ℏ2k22mE = \frac{\hbar^2 k^2}{2m}E=2mℏ2k2​, where k2=kx2+ky2+kz2k^2 = k_x^2 + k_y^2 + k_z^2k2=kx2​+ky2​+kz2​ and ℏ=h2π\hbar = \frac{h}{2\pi}ℏ=2πh​, 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=8mL2h2​(nx2​+ny2​+nz2​).

📌 Key Points
  • ▸

    The energy levels depend on three independent quantum numbers.

  • ▸

    The ground state energy occurs when nx=ny=nz=1n_x=n_y=n_z=1nx​=ny​=nz​=1.

  • ▸

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

  • ▸

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

✅ Advantages
  • ▸

    Predicts discrete energy spectra for confined electrons.

  • ▸

    Explains phenomena like quantum dots and size-dependent bandgaps.

❌ Disadvantages / Limitations
  • ▸

    Assumes an infinite potential barrier, which is an idealization.

  • ▸

    Ignores electron-electron interactions.

🛠️ Applications / Uses
  • ▸

    Quantum Dots and Nanoparticles

  • ▸

    Semiconductor physics

  • ▸

    Statistical mechanics of ideal gases

📄 Additional Information
  • ▸

    For a 1D box, the expression simplifies to E=n2h28mL2E = \frac{n^2 h^2}{8mL^2}E=8mL2n2h2​.

  • ▸

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

  • ▸

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

📊 Diagram / Illustration
Energy Quantization in 3D Box
E=h28mL2×(nx2+ny2+nz2)E = (h^2 / 8mL^2) \times (n_x^2 + n_y^2 + n_z^2)E=8mL2h2​×(nx2​+ny2​+nz2​)
Where nx,ny,nz=1,2,3,...n_x, n_y, n_z = 1, 2, 3, ...nx​,ny​,nz​=1,2,3,...
✅

A is correct — 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 Schrödinger Equation Infinite Potential Well
💡 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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