Ch 4!!! Fundamentals of Quantum Mechanics Flashcards

1
Q

two observations that scienctists in the end of 19th century just couldnโ€™t understand

A
  1. atoms, when inserted in flame, emit light of certain (and not any) colour
    2.heated objects (such as a frying pan) emit light of particular colours, these change with temperatures
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2
Q

how does quantum theory help us

A

most complete theory we have to describe the behaviour of electrons, in turn explains how many biological, physical, and chemical processes work. ex, electronic devices rely on quantum mechanical nature of electrons

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3
Q

diffraction

A

the bending of waves by an obstacle

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4
Q

interference

A

property of all waves, waves interfere with each other and themselves either constructively or destructively

diffraction generally produces concentric circles

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5
Q

concentric circles

A

circles with a common center, in the case of waves this would be the origin

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6
Q

how does diffraction occur

A

as each wave/electron/particle hits atom in crystal lattice, wave splits and itโ€™s components interfere with each other NOT with other electrons

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7
Q

momentum

A

mass x velocity

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8
Q

wavelength

A

distance between nearest points repeating pattern (trough to trough)

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9
Q

de broglieโ€™s equation

A

fancy upside down y h thing = h/p. and p = mv

when fancy thing = wavelength (m)
p = momentum of the particle. kg m s^-1
m = mass of particle in kg
v = velocity of particle in m s^-1. or m/s
h = planckโ€™s constant (6.626 x 10^-34 Js

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10
Q

why can we detect wavelike behaviour in electrons etc, not larger particles like tennis balls??

A

due to the value of h being so small, if you were to divide it by the velocity of a large object you would get a wavelength immensely smaller than the volume of the object being observed. Because of this larger particles do not exhibit observable wavelike properties

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11
Q

how can you maximize diffraction of particles

A

wavelength should be the same as spacing in lattice etc they will be passing through. If smaller than, diffraction will not occur and if greater than, each particle will be diffracted by many atoms etc and the diffraction pattern will be blurred

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12
Q

travelling waves

A

repeating and periodic disturbances that travel from one location to another

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13
Q

what do waves transport??

A

ENERGY not matter, energy that disturbs still medium. Electromagnetic ration transmits energy through oscillating electric and magnetic fields

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14
Q

Definition of a Transverse Wave, how can they be represented??

A

wave which oscillates in direction perpendicular to direction of motion

Amplitude, Wavelength, Frequency

the waves intensity and energy are proportional to the square of itโ€™s amplitude

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15
Q

waves intensity and energy proportional to ___

A

the square of itโ€™s amplitude

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16
Q

amplitude

A

difference between midpoint and crest or trough

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17
Q

wavelength

A

length of one complete cycle, crest to crest or trough to trough

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18
Q

frequency

A

complete cycles the wave can transmit per unit time

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19
Q

speed of wave

A

velocity, unit of distance divided by unit of time

velocity in m s^-1 = frequency (italic v, in s^-1 or Hertz) x wavelength (fancy h y in meters)

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20
Q

EQUATIONS TO KNOW

A

velocity (v) = frequency (italic v) x wavelength

wavelength in m= h(planckโ€™s constant) Js / momentum of a particle in kg m s^-1

Kinetic energy = 1/2 m v^2

momentum in kg m s^-1 = mass of particle (kg) x velocity of particle in m s^-1

E = h^2 n^2 / (8mL^2)

change in energy = h^2 / 8mL^2 x (Ef^2 - Einitial^2)

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21
Q

what happens to the wavelength of a particle when velocity decreases

A

as velocity decreases, momentum decreases and thus wavelength increases

22
Q

basic sin function of a wave

A

f(x) = Asin (2pix/wavelength)

A is a constant, amplitude

23
Q

standing wave

A

bound on either side (length L), appear to be still and do not carry energy from one place to another

24
Q

how can standing wave be formed

A

travelling waves of equal amplitude and frequency but in opposite directions interfere with each other

25
Q

nodes

A

points where amplitude = 0, generally where waves deconstructively interfere with each other

26
Q

where is particle on a wave??

A

it can exist simultaneously everywhere, position can only be predicted - PROBABILITY

27
Q

heisenberg uncertainty principle

A

we cannot know precisely (with zero uncertainty) both the position and momentum of a microscopic particle at the same time

28
Q

particle at rest, velocity momemtum annd KE?

A

all equal to zero

29
Q

probability distribution of particle in a box

A

uniform across length of box, and equal to 1/L

30
Q

remember when predicting average momentum

A

momentum is a VECTOR both magnitude and direction

31
Q

psi (fancy wierd greek y)

A

WAVEFUNCTION - all info that can possibly be obtained from a quantum system in a given state

32
Q

probability distribution of a wave??

A

find by taking the square of the wavefunction

33
Q

schrodinger equation

A

not even going to try to type, google

34
Q

what does potential energy describe

A

ex hydrogen atom n, electron moving in coulomb field of proton, v is PE of the electron from coulombic force between nucleus and electron

PE (V) will depend on the problem

35
Q

schrodinger for particle in a box

A

-h^2/ 8pi^2m x d^2/dx^2 psi = Epsi

d^2/dx^2 psi just means the derivative of the wavefunction

36
Q

wavefunction for quantum particle in a box

A

psi = Asin (kx)

COMPLETE

psi = โˆš(2/L) sin ((npix)/L)

37
Q

n

A

principle quantum number, must equal a positive integer number

38
Q

why canโ€™t n be a fraction?

A

with quantum particle in a box function, psi must equal 0 at L, sin (kL) = 0, this only happens at sin(npi), therefore n can only be a positive integer

39
Q

value of amplitude quantum particle in a box

A

โˆš(2/L)

40
Q

where is the maximum of probability graph?

A

if amplitute psi = โˆš2/L amplitude of wavefunction equals square of this

ex if L = 1 amplitude of prob graph is 2

41
Q

how do you known # of nodes in quantum particle in a box??

A

n - 1

42
Q

equation for energy of particle in a box

A

E = h^2 n^2 / (8mL2)

43
Q

ground state

A

E1 = h^2 / 8mL^2.

LOWEST possible energy

always greater than 0

44
Q

zero point energy

A

difference between the ground state energy and zero

45
Q

excited state

A

any state n>1, so 2, 3, to infinity

n=2 is first excited state

46
Q

how can particles change their energy levels

A

absorbing or emitting energy, ex recieve energy from light or from collisions

47
Q

equation change in energy level

A

change in E = E final - E initial

E final energy of the system in final state (nfinal)

E initial, initial energy original n

change in E = h^2/(8mL^2) x (nfinal^2 -ninitial^2

48
Q

what does change in energy level mean?

A

if positive, system absorbed energy

if negative, system emit energy

49
Q

can particle gain lose completely random amounts of energy??

A

no, quantized, quantum system never observed between states, can only gain or lose exact amounts of energy

50
Q

determining n, wavelength, function (psi), and probability distribution function given # of nodes

A

n = # of nodes + 1

wavelength = 2L/n

function = โˆš(2/L) sin ((n pi x)/L)

probability distribution function = 2/l sin^2((n pi x) /L)

51
Q

how to calculate any excited energy state

A

calculate ground state using h^2 / 8mL^2

multiply this by n^2

52
Q

quantized

A

can only take on certain values