PHYCHEM 2
問題一覧
1
B. The state of a quantum system is represented by a wavefunction, which contains all possible measurements of the system.
2
A. W must be an eigenfunction of A with a corresponding eigenvalue
3
A. The wavefunction collapses into a single eigenfunction corresponding to one of the eigenvalues.
4
C. The uncertainty principle applies, meaning that measuring one observable precisely increases uncertainty in the other.
5
A. a
6
C. h/2
7
B. [x^p^x]=ih
8
A. The wavefunction collapses into the eigenfunction on corresponding to an.
9
A. The same eigenvalue a n with probability 1.
10
A. It determines the shape of the orbital.
11
A. Hermitian operators guarantee that eigenvalues correspond to real physically measurable quantities.
12
C. Any function of a Hermitian operator is alto Hermitian.
13
D. The Hamiltonian operator always commutes with the momentum operator in all systems.
14
C. A must be a Hermitian operator.
15
C. The expectation value of an operator is given by (A)»Ψ-AWdx, even if W is not normalized.
16
A. A particle's position and momentum cannot be measured simultaneously with arbitrary precision because measurement disturbs the system.
17
Α. Δρ >_h/2L
18
B. The square of the expansion coefficient (cn) in the eigenfunction expansion of W.
19
B. It behaves as a free-particle motion.
20
A. Energy levels depend only on n, and states with different I values but the samen are degenerate.
21
B. The hydrogen atom problem.
22
C. It decays exponentially.
23
B.r=a0
24
A. The wavefunction collapses into an eigenstate of Å associated with the measured eigenvalue.
25
B. A spherical surface where the probability density is zero.
26
A. Separation into center-of-mass and relative motion coordinates.
27
C. The electrons independently follow a 1s-orbital distribution similar to hydrogen
28
C. Parahelium has electrons in a singlet spin state, while orthohelium has electrons in a triplet spin state
29
C. n-1-1
30
A. A simple hydrogenic wavefunction for each electron, neglecting electron- electron interactions
31
B)-Z/n^2 RH
32
A) Principal quantum number (n)
33
C) The total wavefunction must be antisymmetric under the exchange of two electrons
34
B) Exchange energy results from the antisymmetry of the total wavefunction and is a purely quantum mechanical effect
35
C) A hydrogen-like Coulomb potential due to the nucleus
36
C) It assumes electrons do not interact with each other
37
A) One electron remains in the 1s orbital while the second electron is excited to a higher orbital
38
B)-3.25RH
39
C) It splits degenerate states into different energy levels
40
C) 1s2s→ 1s2
41
C) It ignores electron-electron repulsion
42
B) It decreases the effective nuclear charge felt by the electrons
43
C) Because electrons are fermions and obey the Pauli Exclusion Principle
44
A) The spatial wavefunction must be symmetric
45
B) To satisfy the Pauli Exclusion Principle
46
C) E=-8RH
47
C) The principal (n), azimuthal (1), magnetic (ml), and spin (ms) quantum numbers
48
B) Orbital angular momentum quantum number I
49
B) Electron-electron interactions and screening effects
50
A) L = 0
51
A) s = 0 for singlet states and s = 1 for triplet states
52
A) deta L = 0 , +- (but not L = 0 -> L = 0 )
53
C) 3d
54
A) It assumes that each electron moves in an average field created by all other electrons.
55
D) L = 1,2
56
D) J = 2, 3, 4
57
B) Electron-electron repulsions significantly modify energy levels.
biochem
biochem
velante · 99問 · 1年前biochem
biochem
99問 • 1年前inorg
inorg
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inorg
100問 • 1年前phychem
phychem
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phychem
99問 • 1年前GREAT BOOKS
GREAT BOOKS
velante · 56問 · 11ヶ月前GREAT BOOKS
GREAT BOOKS
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28問 • 11ヶ月前BIOCHEMZ(glycolysis)
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33問 • 11ヶ月前BIOCHEMZ(krebs)
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32問 • 11ヶ月前BIOCHEMZ(ETC)
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47問 • 11ヶ月前PHYCHEM
PHYCHEM
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FOOD CHEM water charact
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FOOD CHEM starch
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FOOD CHEM starch
46問 • 11ヶ月前FOOD CHEM starch 2
FOOD CHEM starch 2
velante · 18問 · 11ヶ月前FOOD CHEM starch 2
FOOD CHEM starch 2
18問 • 11ヶ月前FOOD CHEM pectins
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FOOD CHEM pectins
42問 • 11ヶ月前ANACHEM m1
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ANACHEM m2
velante · 6問 · 11ヶ月前ANACHEM m2
ANACHEM m2
6問 • 11ヶ月前ANACHEM m3
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ANACHEM m3
21問 • 11ヶ月前branches of ethics
branches of ethics
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branches of ethics
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branches of philosophy
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branches of philosophy
13問 • 10ヶ月前morality
morality
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morality
33問 • 10ヶ月前greeks
greeks
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greeks
13問 • 10ヶ月前chap 20
chap 20
velante · 10問 · 9ヶ月前chap 20
chap 20
10問 • 9ヶ月前chapt 21A
chapt 21A
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chapt 21A
10問 • 9ヶ月前chapt 21B
chapt 21B
velante · 10問 · 9ヶ月前chapt 21B
chapt 21B
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chapt 22
velante · 10問 · 9ヶ月前chapt 22
chapt 22
10問 • 9ヶ月前chapt 23A
chapt 23A
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chapt 23A
10問 • 9ヶ月前chapt 23B
chapt 23B
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chapt 23B
10問 • 9ヶ月前chapt 24
chapt 24
velante · 10問 · 9ヶ月前chapt 24
chapt 24
10問 • 9ヶ月前identi
identi
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identi
10問 • 9ヶ月前application
application
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application
5問 • 9ヶ月前matching
matching
velante · 10問 · 9ヶ月前matching
matching
10問 • 9ヶ月前multiple choices
multiple choices
velante · 20問 · 9ヶ月前multiple choices
multiple choices
20問 • 9ヶ月前問題一覧
1
B. The state of a quantum system is represented by a wavefunction, which contains all possible measurements of the system.
2
A. W must be an eigenfunction of A with a corresponding eigenvalue
3
A. The wavefunction collapses into a single eigenfunction corresponding to one of the eigenvalues.
4
C. The uncertainty principle applies, meaning that measuring one observable precisely increases uncertainty in the other.
5
A. a
6
C. h/2
7
B. [x^p^x]=ih
8
A. The wavefunction collapses into the eigenfunction on corresponding to an.
9
A. The same eigenvalue a n with probability 1.
10
A. It determines the shape of the orbital.
11
A. Hermitian operators guarantee that eigenvalues correspond to real physically measurable quantities.
12
C. Any function of a Hermitian operator is alto Hermitian.
13
D. The Hamiltonian operator always commutes with the momentum operator in all systems.
14
C. A must be a Hermitian operator.
15
C. The expectation value of an operator is given by (A)»Ψ-AWdx, even if W is not normalized.
16
A. A particle's position and momentum cannot be measured simultaneously with arbitrary precision because measurement disturbs the system.
17
Α. Δρ >_h/2L
18
B. The square of the expansion coefficient (cn) in the eigenfunction expansion of W.
19
B. It behaves as a free-particle motion.
20
A. Energy levels depend only on n, and states with different I values but the samen are degenerate.
21
B. The hydrogen atom problem.
22
C. It decays exponentially.
23
B.r=a0
24
A. The wavefunction collapses into an eigenstate of Å associated with the measured eigenvalue.
25
B. A spherical surface where the probability density is zero.
26
A. Separation into center-of-mass and relative motion coordinates.
27
C. The electrons independently follow a 1s-orbital distribution similar to hydrogen
28
C. Parahelium has electrons in a singlet spin state, while orthohelium has electrons in a triplet spin state
29
C. n-1-1
30
A. A simple hydrogenic wavefunction for each electron, neglecting electron- electron interactions
31
B)-Z/n^2 RH
32
A) Principal quantum number (n)
33
C) The total wavefunction must be antisymmetric under the exchange of two electrons
34
B) Exchange energy results from the antisymmetry of the total wavefunction and is a purely quantum mechanical effect
35
C) A hydrogen-like Coulomb potential due to the nucleus
36
C) It assumes electrons do not interact with each other
37
A) One electron remains in the 1s orbital while the second electron is excited to a higher orbital
38
B)-3.25RH
39
C) It splits degenerate states into different energy levels
40
C) 1s2s→ 1s2
41
C) It ignores electron-electron repulsion
42
B) It decreases the effective nuclear charge felt by the electrons
43
C) Because electrons are fermions and obey the Pauli Exclusion Principle
44
A) The spatial wavefunction must be symmetric
45
B) To satisfy the Pauli Exclusion Principle
46
C) E=-8RH
47
C) The principal (n), azimuthal (1), magnetic (ml), and spin (ms) quantum numbers
48
B) Orbital angular momentum quantum number I
49
B) Electron-electron interactions and screening effects
50
A) L = 0
51
A) s = 0 for singlet states and s = 1 for triplet states
52
A) deta L = 0 , +- (but not L = 0 -> L = 0 )
53
C) 3d
54
A) It assumes that each electron moves in an average field created by all other electrons.
55
D) L = 1,2
56
D) J = 2, 3, 4
57
B) Electron-electron repulsions significantly modify energy levels.