Quantum Mechanics 101 · Unit 3: The Mathematical Machinery
Quantum Academy · Chapter 10: The Schrödinger Equation
The engine that moves the wavefunction through time
Part A Vocabulary matching
Write the letter of the matching definition in the blank beside each term.
- 1.Schrödinger equation
- 2.Hamiltonian
- 3.Operator
- 4.Partial derivative
- 5.Curvature
- 6.Potential energy function
- 7.Eigenvalue equation
- 8.Stationary state
- 9.Superposition principle
- 10.Group velocity
- 11.Dispersion
- 12.Boundary conditions
- A.The speed of a wave packet's envelope, dω/dk; for a free particle it equals p/m.
- B.Requirements at edges, walls and infinity, such as ψ → 0 or continuity, that select the physically allowed solutions.
- C.The total-energy operator Ĥ, kinetic plus potential; it drives the time evolution of ψ.
- D.How sharply a graph bends, measured by its second derivative; for ψ it tracks kinetic energy.
- E.A definite-energy solution whose probability density and averages do not change in time.
- F.The spreading of a wave packet because its component waves travel at different speeds.
- G.The rate of change of a function of several variables with respect to one of them while the others are held fixed.
- H.An equation like Ĥφ = Eφ, in which an operator returns the same function multiplied by a number, the eigenvalue.
- I.A rule that turns one function into another, such as 'take the second derivative' or 'multiply by V(x)'.
- J.V(x), the energy a particle would have at each position because of the forces on it: the landscape ψ moves through.
- K.The equation of motion for the wavefunction, iħ ∂ψ/∂t = Ĥψ; it fixes how ψ changes in time.
- L.Because the equation is linear, any weighted sum of solutions is also a solution.
Part B Questions
- 1.
In iħ ∂ψ/∂t = Ĥψ, what does the Hamiltonian operator Ĥ represent?Circle one
- AThe particle's momentum
- BThe total energy, kinetic plus potential
- CThe probability of finding the particle
- DThe measuring apparatus
- 2.
In the same region, wavefunction A has many tight wiggles while wavefunction B is a long, gentle wave. Which statement is correct?Circle one
- AA has more potential energy
- BB has more kinetic energy
- CA has more kinetic energy
- DThey must have equal kinetic energy
- 3.
The time-dependent Schrödinger equation contains a random term that makes ψ jump unpredictably.Circle one
TrueFalse
- 4.
If ψ₁ and ψ₂ both solve the time-dependent Schrödinger equation for the same potential, then 0.6ψ₁ + 0.8iψ₂ is also a solution.Circle one
TrueFalse
- 5.
A solution of definite energy whose probability density never changes in time is called a state.Fill in the blank
- 6.
The centre of a free wave packet moves at the velocity, which equals p/m.Fill in the blank
- 7.
Explain why multiplying a spatial shape φ(x) by the phase factor e^(−iEt/ħ) leaves the probability density unchanged in time.Short answer
- 8.
Why does requiring ψ to be normalizable lead to discrete energy levels for a particle bound in a well?Short answer
- 9.
Hydrogen's ground state is a stationary state. Give two reasons it is nevertheless wrong to say the electron is sitting still.Short answer
- 10.
An electron wave packet has a central de Broglie wavelength of 0.50 nm and moves in free space. How far does its centre move in 2.0 fs?Show your working
WorkingAnswer:
- 11.
A free electron plane wave has wavenumber k = 1.0×10¹⁰ m⁻¹. Use the Schrödinger equation's result E = ħ²k²/2m to find its energy in eV and its group velocity.Show your working
WorkingAnswer:
- 12.
A hydrogen atom is placed in a superposition of its n = 2 and n = 3 levels (E₂ = −3.40 eV, E₃ = −1.51 eV). At what frequency does its probability cloud oscillate? Compare with the Balmer line from n = 3 to n = 2.Show your working
WorkingAnswer:
- 13.
An electron is localized in a Gaussian packet of width σ₀ = 1.0 nm. Find the spreading time τ = 2mσ₀²/ħ and the packet's width after 1.0 ps.Show your working
WorkingAnswer:
Part C Mad scientist challenge bonus
The sloshing electron. An electron is trapped in a box 1.0 nm wide whose two lowest stationary states have real spatial shapes φ₁(x) and φ₂(x) and energies E₁ = 0.376 eV and E₂ = 1.504 eV (you will derive these in Chapter 11). At t = 0 it is prepared in ψ = (φ₁ + φ₂)/√2. (a) Write ψ(x, t). (b) Show that |ψ|² = ½φ₁² + ½φ₂² + φ₁φ₂ cos(ΔE·t/ħ), where ΔE = E₂ − E₁. (c) Is this a stationary state? Describe what the probability does, given that φ₁ is symmetric about the box's centre and φ₂ is antisymmetric. (d) Find the period of the motion. (e) What photon wavelength carries the same energy difference?