Intermolecular Forces and Potentials Flashcards

1
Q

Van der Waals

A

non-covalent interactions

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2
Q

force

A

vector

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3
Q

Positive Q

A

attractive

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4
Q

Negative Q

A

repulsive

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5
Q

Multipole moment of heterodiatomic

A

quadrupole, accumulation of e- density between the nuclei

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6
Q

monopole

A

point charge

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7
Q

dipole

A

superposition of 2 monopoles with opposite charges

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8
Q

quadrupole

A

superposition of 2 oppositely oriented dipoles

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9
Q

Components of intermolecular potential

A

dipole A - dipole B, dipole A - quad B, quad A - dipole B, quad A - quad B

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10
Q

Distance dependence of monopole-monopole

A

r-1

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11
Q

Distance dependence of monopole-dipole

A

r-2

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12
Q

Distance dependence of monopole-quadrupole

A

r-3

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13
Q

Distance dependence of dipole-dipole

A

r-3

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14
Q

Distance dependence of dipole-quadrupole

A

r-4

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15
Q

Distance dependence of quadrupole-quadrupole

A

r-5

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16
Q

Orientation of multipoles

A

orientations sampled with probability that reflects their energy ie. use boltzmann

17
Q

Dipole-dipole interactions

A

also called Keesom, attractive or repulsive depending on orientation, molecules don’t rotate freely at finite temp, attractive orientations more favoured than repulsive interactions

18
Q

Induction interactions

A

always attractive, permanent multipole of A induces permanent multipole on B, magnitude depends on magnitude of multipole of A and polarisability of B, not frustrated by thermal motion

19
Q

Dispersion interactions

A

also called London Dispersion, always attractive, instantaneous multipole of A correlate with instantaneous multipole of B, not frustrated by thermal motion

20
Q

Origin of dispersion interactions

A

electrons in constant motion so can have instantaneous dipole moment, this induces another dipole in adjacent atom giving an attractive potential

21
Q

Magnitude of polarisability volumes

A

similar in magnitude to actual molecular volumes, correlates with HOMO-LUMO separation in atoms/molecules, electron distribution distorted easily if LUMO and HOMO are close in energy

22
Q

Dipoles at low AC frequency

A

dipoles have time to re-orient themselves with oscillating electric field, can contribute to dielectric constant, use Debye equation to interpret temp dependence of molar polarisation

23
Q

Dipoles at high AC frequency

A

dipoles can’t keep up with oscillating freq, can’t contribute to dielectric const, molar polarisation independent of temp and use mossotti to determine polarisability

24
Q

Stark deceleration

A

molecule with permanent dipole approaches dipole and slows due to increasing field, reaches position at top of energy hill, fields switched to prevent molecule continuing down hill, voltage of first and second electrode swapped, molecule instantaneously arrives at bottom of hill and continues climbing but slower, repeated until desired velocity reached

25
Repulsive wall contributions
nuclear-nuclear repulsion, electron-nucleus repulsion and electron-electron repulsion
26
Valence repulsion
atoms with closed shells repel each other, valence repulsion due to overlap of orbitals of interacting molecules, overlap decays exp with increasing molecular distance
27
which interactions are additive
electrostatic only