QM 1 - translational, vibrational, rotational motion

0.0(0)
Studied by 0 people
call kaiCall Kai
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/35

encourage image

There's no tags or description

Looks like no tags are added yet.

Last updated 11:21 AM on 4/19/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai

No analytics yet

Send a link to your students to track their progress

36 Terms

1
New cards
<p>explain the difference between free translation and confined translation</p>

explain the difference between free translation and confined translation

free = constant speed, no interactions, any energy (not quantised)

confined = energy is restricted to certain values, interactions with wall

2
New cards

for free translational motion - what is potential and kinetic energy?

no interactions = nothing to slow it down, speed it up or change direction of motion

no potential energy, energy is purely kinetic

<p>no interactions = nothing to slow it down, speed it up or change direction of motion </p><p>no potential energy, energy is purely kinetic </p>
3
New cards
<p>what is the Schrodinger equation for free translational motion?2</p>

what is the Schrodinger equation for free translational motion?2

can be written as linear combination or as sine and cosine

<p>can be written as linear combination or as sine and cosine </p>
4
New cards
<p>what does this mean?</p>

what does this mean?

there is no restriction, k can be any non negative real number

all energies are allowed -free translational motion is not quantised

5
New cards
<p>explain what it means if k = 0, and if k&gt;0</p><p>for free translational motion, show energy vs momentum graph</p><p>explain what graph shows</p>

explain what it means if k = 0, and if k>0

for free translational motion, show energy vs momentum graph

explain what graph shows

if k = 0 the particle is still

if k > 0 , the particle is moving and energy equals as shown

  • graph shows energy and momentum vary smoothly and continuously = shows no restrictions on k

<p>if k = 0 the particle is still</p><p>if k &gt; 0 , the particle is moving and energy equals as shown</p><ul><li><p>graph shows energy and momentum vary smoothly and continuously = shows no restrictions on k </p></li></ul><p></p>
6
New cards

what are the conditions of the box for particle in a box?

potential energy is 0 inside the box

box length is L

walls are infinitely repulsive (potential energy suddenly shoots up to ∞). this means no transfer of E to the wall

  • the wall is infinitely hard = no bounce back/deformation

7
New cards
<p>what are the values of these operators?</p>

what are the values of these operators?

same as in free translation

  • purely kinetic

8
New cards

what does infinite repulsion mean about boundary conditions for particle in a box?

at the walls (x=0 and x=L), the wavefunction must equal 0

  • particle cannot be found there

  • this means that |ψ|2 = 0 and ψ = 0

<p>at the walls (x=0 and x=L), the wavefunction must equal 0</p><ul><li><p>particle cannot be found there</p></li><li><p>this means that |ψ|<sup>2</sup> = 0 and ψ = 0</p></li></ul><p></p>
9
New cards
<p>what is the consequence of these boundary conditions?</p>

what is the consequence of these boundary conditions?

not every wavelength fits properly between the walls

  • must be a sine function that starts at 0, oscillates and then returns to 0 at x=L

  • must be a whole number of half-wavelengths

this leads to quantisation

<p>not every wavelength fits properly between the walls </p><ul><li><p>must be a sine function that starts at 0, oscillates and then returns to 0 at x=L</p></li><li><p>must be a whole number of half-wavelengths </p></li></ul><p>this leads to quantisation </p><p></p>
10
New cards
<p>what is n? what is N?</p>

what is n? what is N?

n is the quantum number (can only take positive integer values)

  • the value of n is the same as the number of half wavelengths the wavefunction has

N is the normalisation constant

11
New cards

show diagram of particle in a box wavefunctions for each quantum number up to n = 4

knowt flashcard image
12
New cards
<p>explain why cos term is not involved in particle in a box and how this is achieved </p>

explain why cos term is not involved in particle in a box and how this is achieved

ψ=0 when x =0 but cos(0)=1

M = 0 to maintain this

13
New cards
<p>explain how the red and green wavelengths are incorrect</p>

explain how the red and green wavelengths are incorrect

the wavelength of red is too long as it hasnt completed enough oscillations by the time it gets to x=L

  • there is a discontinuity at x=L as it doesnt hit zero

the wavelength of green is too short, it oscillates too quickly and doesnt land on 0 when x=L

  • this leads to a discontinuity

wavelengths must be continuous

14
New cards
<p>explain how the wavelengths not being continuous leads to quantisation of energy</p>

explain how the wavelengths not being continuous leads to quantisation of energy

only some wavelengths being acceptable

since wavelength is connected to momentum through the de Broglie equation (p=h/λ)

momentum is connected to KE (K=p2/2m)

  • restricting wavelengths means restricting energy

15
New cards

what is the ground state for particle in a box

n =1

no nodes, single arch - 1 half wavelength

16
New cards
<p>what happens as n increases? 3</p>

what happens as n increases? 3

number of nodes (n-1) increases

curvature of ψ increases, λ decreases, K increases

correspondence principle

17
New cards

why does KE increase as n increases in particle in a box?

the more curved the function is the more KE

the components are moving faster

18
New cards

what is the correspondence principle for particle in a box?

non uniformity of |ψ|2 becomes harder to detect

  • as you go macroscopic, there is constant probability of finding the particle anywhere in the box

quantum mechanics resembles classical - spends equal time everywhere

19
New cards

what is the zero point energy of particle in a box?

the lowest energy

  • confined particle can never stay still

20
New cards

why is the zero point energy not zero?

explain in terms of uncertainty and wavefunction shape

the uncertainty principle says that as the uncertainty of x is finite (confined to region of finite size), the uncertainty of p cannot be zero. if momentum isnt precisely zero, KE cant be zero either

the wavefunction must be zero at the walls but it cannot be zero everywhere (zero probability of finding the particle in the box)

  • wavefunction must be curved which means KE

<p>the uncertainty principle says that as the uncertainty of x is finite (confined to region of finite size), the uncertainty of p cannot be zero. if momentum isnt precisely zero, KE cant be zero either </p><p></p><p>the wavefunction must be zero at the walls but it cannot be zero everywhere (zero probability of finding the particle in the box)</p><ul><li><p>wavefunction must be curved which means KE</p></li></ul><p></p>
21
New cards

how do the energy gaps change as you go up in particle in a box? why?

energy gaps increase with n

gap between n and n+1 is proportional to 2n+1

  • the potential rises more steeply than the potential of a harmonic oscillator (which has constant gaps)

22
New cards

what is the energy gap and ZPE of particle in a box proportional to?

what about for macroscopic?

h2/mL2 (energy scale)

  • this gives energies that matter for electron in box the size of a chemical bond

for macroscopic, it is too small to be observed

  • dont notice quantisation when looking at macroscopic

<p>h<sup>2</sup>/mL<sup>2 </sup>(energy scale)</p><ul><li><p>this gives energies that matter for electron in box the size of a chemical bond</p></li></ul><p>for macroscopic, it is too small to be observed</p><ul><li><p>dont notice quantisation when looking at macroscopic</p></li></ul><p></p>
23
New cards
<p>explain what this shows</p><ul><li><p>electron in 100 pm box vs marble in 10 cm box</p></li></ul><p></p>

explain what this shows

  • electron in 100 pm box vs marble in 10 cm box

for electron, the ZPE is a few million joules per mole. the energy gap between 2 and 1 is 3x that - these are chemically significant

for the marble, the ZPE is much smaller (of the order of 10-40 Jmol-1) and undetectably small. the energy gap is also essentially zero. energies so small cannot be detected

  • quantisation is there in principle but for macroscopic, the ELs are so close together that they form what looks like a continuous spectrum

= correspondence principle

24
New cards

when is separation of variables applicable?

when the Hamiltonian is a sum of independent terms

  • coordinates that appear in one term do not appear in any other

<p>when the Hamiltonian is a sum of independent terms </p><ul><li><p>coordinates that appear in one term do not appear in any other </p></li></ul><p></p>
25
New cards

what is the wavefunction for a particle in a two or three dimensional box?

product of wavefunctions for a particle in a one dimensional box

26
New cards

what is the energy of a particle in a two or three dimensional box?

sum of the energies for each one dimensional component

27
New cards
<p>for a particle in a 1D box - what is the Hamiltonian? what does the energy depend on? and what is the wavefunction?</p>

for a particle in a 1D box - what is the Hamiltonian? what does the energy depend on? and what is the wavefunction?

hamiltonian is the KE operator (second derivative wrt to x)

energy depends on a single quantum number n

wavefunction is a sin function with x as its variable

28
New cards
<p>for a particle in a 2D box - what is the Hamiltonian? is the separation of variables applicable? what is the energy? what is the wavefunction? how many quantum numbers?</p>

for a particle in a 2D box - what is the Hamiltonian? is the separation of variables applicable? what is the energy? what is the wavefunction? how many quantum numbers?

hamiltonian has two KE terms - one involving the second derivative wrt x and the other involving the second derivative wrt y

separation of variables is applicable

  • the two terms are independent and dont interfere with each other

  • 2D can be split into a pair of 1D problems

since separation of variables is applicable, the total E is a sum of two independent 1D energies

wavefunction is a product of two independent 1D wavefunctions

there is now two quantum numbers, one for each dimension

29
New cards

show the Schrödinger equation for 3 dimensions

knowt flashcard image
30
New cards

show particle in a 1D box wavefunctions (n=1 and n=2 overlayed) and explain positive and negative lobes

ground state has a single arch and is positive everywhere in the box

the wavefunction of the first excited state has a node in the middle and has one positive and one negative lobe

<p>ground state has a single arch and is positive everywhere in the box </p><p>the wavefunction of the first excited state has a node in the middle and has one positive and one negative lobe </p>
31
New cards

show particle in a 2D box wavefunctions for nx=1 or 2 and ny=1 or 2

explain the lobes

for ground state (nx=ny=1) there is a single positive region

nx=2 and ny=1 there is a quantum of excitation in x, there is a vertical nodal line at x=Lx/2

nx=1 and ny=2 there is a quantum of excitation in the y direction so there is a horizontal nodal line at y=Ly/2

for nx=ny=2 there are nodes in both directions which creates a pattern of 4 lobes with alternating signs

<p>for ground state (n<sub>x</sub>=n<sub>y</sub>=1) there is a single positive region </p><p>n<sub>x</sub>=2 and n<sub>y</sub>=1 there is a quantum of excitation in x, there is a vertical nodal line at x=L<sub>x</sub>/2</p><p>n<sub>x</sub>=1 and n<sub>y</sub>=2 there is a quantum of excitation in the y direction so there is a horizontal nodal line at y=L<sub>y</sub>/2</p><p>for n<sub>x</sub>=n<sub>y</sub>=2 there are nodes in both directions which creates a pattern of 4 lobes with alternating signs </p>
32
New cards

for a square box where Lx=Ly=L, what is the energy formula?

knowt flashcard image
33
New cards
<p>show whether (n<sub>x</sub>,n<sub>y</sub>)=(3,3) is degenerate or not</p><p>show diagram</p>

show whether (nx,ny)=(3,3) is degenerate or not

show diagram

there is only one state where you can get 18

<p>there is only one state where you can get 18 </p>
34
New cards
<p>show whether (n<sub>x</sub>,n<sub>y</sub>)=(1,2) and (n<sub>x</sub>,n<sub>y</sub>)=(2,1) are degenerate or not</p><p>show diagram</p>

show whether (nx,ny)=(1,2) and (nx,ny)=(2,1) are degenerate or not

show diagram

nx2+ny2=5 in both cases

there is symmetry in the box so if you rotate by 90 degrees, you swap the x and y directions and the wavefunctions transform into each other

  • the wavefunctions have the same energy if excitation along x or y

<p>n<sub>x</sub><sup>2</sup>+n<sub>y</sub><sup>2</sup>=5 in both cases </p><p>there is symmetry in the box so if you rotate by 90 degrees, you swap the x and y directions and the wavefunctions transform into each other </p><ul><li><p>the wavefunctions have the same energy if excitation along x or y  </p></li></ul><p></p>
35
New cards
<p>give an example of accidental degeneracy (for example use n<sub>x</sub><sup>2</sup>+n<sub>y</sub><sup>2</sup>=50)</p><p>show diagram</p>

give an example of accidental degeneracy (for example use nx2+ny2=50)

show diagram

(7,1)/(1,7) and (5,5) are not related to each other by symmetry but they are degenerate as they have the same energy

<p>(7,1)/(1,7) and (5,5) are not related to each other by symmetry but they are degenerate as they have the same energy </p>
36
New cards