Practice Midterm Flashcards

1
Q

A valid wavefunction must be single-valued and not go to infinity

A

True
(must be single-valued and not go to infinity)

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2
Q

A valid wavefunction must be an eigenfunction of the Hamiltonian

A

False
(A valid wavefunction does not have to be an eigenfunction of the Hamiltonian)

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3
Q

The eigenvalues of a Hermitian operator must be real numbers

A

True
(MUST BE REAL #’S)

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4
Q

The eigenfunctions of a nondegenerate Hermitian Operator must be orthogonal

A

True
(Hermitian = orthogonal)

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5
Q

Nondegenerate

A

quantum states that have unique energy levels, meaning that no two states share the same energy value

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6
Q

The most probable location of a particle in a box is always L/2

A

False
(depends on energy & quantum number)

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7
Q

For a particle in a box in a stationary state <p>=0

A

True
(momentum cancels itself out)

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8
Q

If [A,B] = 0, then A and B must have the same eigenfunctions

A

False.

(If they commute, they can share a common set, but not necessarily having same e-functions)

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9
Q

Any valid wavefunction can be constructed using the eigenfunctions of a Hermitian operator.

A

True.
(Hermitian is good, so yes)

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10
Q

A small particle will behave classically when it has low kinetic energy.

A

False.

(Reverse. remember the amount of oscillations and nodes contributing to a straiter line)

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11
Q

The energy of a rigid rotor depends on both quantum numbers l and m.

A

False
(depends on l more than m)

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12
Q

Kinetic Energy equals

A

(3/2)kB *T

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13
Q

Kinetic Energy equals

A

(1/2)mv^2

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14
Q

mass of electron

A

9.11 x 10^-31

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15
Q

If particles travel at the same energy, they must have the same de Broglie wavelength.

A

False
(need to have the same mass)

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16
Q

The expectation value <x> gives the most probable location for the particle in a box</x>

A

False
(average position not most probable)

17
Q

A valid wavefunction must satisfy integral |Psi(x)|^2 = 1

A

True
(needs to satisfy the normalization condition, total probability of finding the particle somewhere in space is 1)

18
Q

The Heisenburg representation of a wavefunction is a matrix.

A

False (they are state vectors)

19
Q

The eigenfunctions of the Hamiltonian are the only possible quantum states of the system.

A

False
(they represent stationary states, not superpositions)

20
Q

A well-behaved wavefunction cannot go to infinity on the interval where it is defined.

A

True
(A well-behaved wavefunction must be finite - not go to infinity)

21
Q

A superposition state is also called a nonstationary state.

A

True.
(unlike a single energy eigenstate, a superposition of multiple eigenstates generally results in time-dependent behavior - leading to a nonstationary state)

22
Q

The nondegenerate eigenstates of a Hermitian operator must be orthogonal (by default)
.

A

True.
(Follows properties of Hermitian operators, guarantee the eigenstates corresponding to different eigenvalues are orthogonal)

23
Q

The eigenfunctions of the rigid rotor Hamiltonian are non degenerate.

A

False
(They exhibit degeneracy. E-values are nondegenerate for l, but the E-Functions are degenerate)

24
Q

If two operators commute, there will be an uncertainty relation between their observables.

A

False
(There is no uncertainty. Heisenburg Uncertainty principle applies to non-commuting observables).

25
Q

If two particles travel at the same velocity, they must have the same deBroglie wavelength.

A

False

(differing masses could travel at same v)

26
Q

All Hermitian operators are real.

A

False.

(not necessarily real-valued operators themselves)

27
Q

All eigenvalues of a Hermitian operator is a diagonal matrix

A

False
(doesn’t have to be, only diagonal if the basis set is eigenfunction of Hermetian operator)

28
Q

An eigenfunction of the Hamiltonian is also called a stationary state.

A

True
(Eigen function of Hamiltonian is stationary state)

29
Q

A well-behaved wavefunction must have only real values.

A

False.

(spherical harmonics have an imaginary part)

30
Q

An eigenfunction of the Hamiltonian is also called a stationary state.

A

True.

31
Q

The non-degenerate eigenstates of a Hermitian operator must be orthogonal.

A

True.

(Hermitian is usually pretty nice to work with, so you can assume orthogonality works)

32
Q

A valid wavefunction must be normalized.

A

True.
(Physically, the total probability of the particle existing must equal to 1)

33
Q

If two operators commute, there will be an uncertainty relation between their observables.

A

False.

(There is no uncertainty relation. Only uncertainty when they don’t commute!)