Circus of Physics

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Most Probable Radius of 1s Electron in Hydrogen Atom Explained | Modern Physics Problem 6.15 Beiser
Most Probable Radius of 1s Electron in Hydrogen Atom Explained | Modern Physics Problem 6.15 Beiser
When Is an Atomic Electron’s Probability Density Spherically Symmetric? | Quantum Mechanics Explain
When Is an Atomic Electron’s Probability Density Spherically Symmetric? | Quantum Mechanics Explain
Percentage Difference Between L and Maximum Lz for p, d & f Atomic Orbitals | Arthur Beiser Physics
Percentage Difference Between L and Maximum Lz for p, d & f Atomic Orbitals | Arthur Beiser Physics
Quantum Numbers for n = 4 Hydrogen Atom | Arthur Beiser Modern Physics Solved
Quantum Numbers for n = 4 Hydrogen Atom | Arthur Beiser Modern Physics Solved
Magnetic Quantum Number ml Values for l=4 | Magnetic Quantum Number Explained |Beiser Modern Physics
Magnetic Quantum Number ml Values for l=4 | Magnetic Quantum Number Explained |Beiser Modern Physics
Angles Between Orbital Angular Momentum (L) and z-Axis for l=1 & l=2 | Quantum Physics Problem
Angles Between Orbital Angular Momentum (L) and z-Axis for l=1 & l=2 | Quantum Physics Problem
When Can Lz ​=L? | When Angular-Momentum Component Equals Total Angular Momentum?
When Can Lz ​=L? | When Angular-Momentum Component Equals Total Angular Momentum?
Particle on a Ring | Schrödinger Equation, Energy & Angular Momentum Solutions | Arthur Beiser Ch. 6
Particle on a Ring | Schrödinger Equation, Energy & Angular Momentum Solutions | Arthur Beiser Ch. 6
Angular Momentum of a Ground-State Electron: Bohr Model vs Quantum Theory | Modern Physics Solved
Angular Momentum of a Ground-State Electron: Bohr Model vs Quantum Theory | Modern Physics Solved
Normalization of Hydrogen Azimuthal Wavefunction Φ(φ)=A e^{imₗ φ} Prove A = 1/√(2π) | Beiser Quantum
Normalization of Hydrogen Azimuthal Wavefunction Φ(φ)=A e^{imₗ φ} Prove A = 1/√(2π) | Beiser Quantum
Verify Orthogonality of Azimuthal Wave Functions | Hydrogen Atom | Evaluate ∫₀²π Φₘℓ* Φₘ′ℓ dφ
Verify Orthogonality of Azimuthal Wave Functions | Hydrogen Atom | Evaluate ∫₀²π Φₘℓ* Φₘ′ℓ dφ
R21(r) Radial Wave-function Solution & Normalization Proof | Modern Physics Eq. (6.14) Beiser
R21(r) Radial Wave-function Solution & Normalization Proof | Modern Physics Eq. (6.14) Beiser
Proof & Normalization of R₁₀(r) Radial Wavefunction | R₁₀(r) = (2/a₀³ᐟ²) e^(–r/a₀) Solves Eq. (6.14)
Proof & Normalization of R₁₀(r) Radial Wavefunction | R₁₀(r) = (2/a₀³ᐟ²) e^(–r/a₀) Solves Eq. (6.14)
Beiser Modern Physics | Proving & Normalizing Θ₂₀(θ)=√10/4(3cos²θ–1) | Step-by-Step Solution
Beiser Modern Physics | Proving & Normalizing Θ₂₀(θ)=√10/4(3cos²θ–1) | Step-by-Step Solution
Why Are Three Quantum Numbers Needed to Describe an Atomic Electron? | Arthur Beiser Concepts
Why Are Three Quantum Numbers Needed to Describe an Atomic Electron? | Arthur Beiser Concepts
Harmonic Oscillator Ψ₃ Wave Function Proved | Schrödinger Equation Solution (Beiser Ch. 5)
Harmonic Oscillator Ψ₃ Wave Function Proved | Schrödinger Equation Solution (Beiser Ch. 5)
Prove Ψ₂(x) Solves the Schrödinger Equation for the 1D Quantum Harmonic Oscillator | Beiser Example
Prove Ψ₂(x) Solves the Schrödinger Equation for the 1D Quantum Harmonic Oscillator | Beiser Example
Prove Ψ₁(x) Solves the Schrödinger Equation for the 1D Quantum Harmonic Oscillator | Beiser solution
Prove Ψ₁(x) Solves the Schrödinger Equation for the 1D Quantum Harmonic Oscillator | Beiser solution
Zero-Point Energy & Quantum Number of a 1-gram Pendulum | Modern Physics Solved (Beiser)
Zero-Point Energy & Quantum Number of a 1-gram Pendulum | Modern Physics Solved (Beiser)
Expectation Value of Potential & Kinetic Energy in Quantum Harmonic Oscillator (n=0) | Beiser Solved
Expectation Value of Potential & Kinetic Energy in Quantum Harmonic Oscillator (n=0) | Beiser Solved
Expectation Values ⟨x⟩ & ⟨x²⟩ | Harmonic Oscillator States n=0 & n=1 | Beiser Modern Physics Solved
Expectation Values ⟨x⟩ & ⟨x²⟩ | Harmonic Oscillator States n=0 & n=1 | Beiser Modern Physics Solved
Harmonic Oscillator Ground-State Probability Density |Ψ₀|² at x = 0, ±A | Modern Physics Solved
Harmonic Oscillator Ground-State Probability Density |Ψ₀|² at x = 0, ±A | Modern Physics Solved
Harmonic Oscillator n=0 State: Proving y=1 at x=A | Show Harmonic Oscillator n=0 State Amplitude
Harmonic Oscillator n=0 State: Proving y=1 at x=A | Show Harmonic Oscillator n=0 State Amplitude
Minimum Energy of a Quantum Harmonic Oscillator from Δx & Δp | ½hν Proof | Beiser Modern Physics
Minimum Energy of a Quantum Harmonic Oscillator from Δx & Δp | ½hν Proof | Beiser Modern Physics
Zero-Point Energy & Heisenberg Uncertainty Principle in Harmonic Oscillator | Arthur Beiser Solved
Zero-Point Energy & Heisenberg Uncertainty Principle in Harmonic Oscillator | Arthur Beiser Solved
Correspondence Principle & Harmonic Oscillator | Energy-Level Spacing Ratio ΔEₙ/Eₙ Explained
Correspondence Principle & Harmonic Oscillator | Energy-Level Spacing Ratio ΔEₙ/Eₙ Explained
Quantum Tunneling: Energy for 1% Transmission (6.00 eV Barrier, 0.200 nm) | Beiser Eq. 5.60
Quantum Tunneling: Energy for 1% Transmission (6.00 eV Barrier, 0.200 nm) | Beiser Eq. 5.60
Quantum Tunneling Explained: 0.400 eV Electrons vs 3.00 eV Barrier | Modern Physics Solved
Quantum Tunneling Explained: 0.400 eV Electrons vs 3.00 eV Barrier | Modern Physics Solved
Ground-State Energy of a Particle in a Box (1D vs 3D) | Particle in a 1D & 3D Box | Energy Levels
Ground-State Energy of a Particle in a Box (1D vs 3D) | Particle in a 1D & 3D Box | Energy Levels
3D Particle in a Box | Probability in L/4 & L/2 Cubes | Modern Physics Solved Step-by-Step
3D Particle in a Box | Probability in L/4 & L/2 Cubes | Modern Physics Solved Step-by-Step