Quantum Physics Flashcards

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1
Q

Gauss Law

faradays law

both are dot

A

the total electric flux out of a closed surface (area) is equal to the charge enclosed divided by the permittivity

the electric flux through a closed surface is proportional to the net electric charge enclosed by the surface

faradays law

The electromotive force around a closed path is equal to the negative of the rate of change of the magnetic flux enclosed by the path.

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2
Q

Gauss law of magnetism
Ampere-Maxwell law:
both are cross

A

the net magnetic flux of the magnetic field must always be zero over any closed surface. (area)
AMPERE MAXWELL
The total current passing through any surface of which the closed loop is is the sum of the conduction current and the rate of displacement current.

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3
Q

Gauss law formula

Fardays law formula

Gauss Magnetic formula

Maxwell ampere formula

properties of EM WAVES

A

∇.E = P/εo

∇ . E = - ∂B/∂t

∇XB=0

∇XE = J (μ+ ∂D/∂t)

1) Vibrations of E & B
2) fields through free space at speed C
3) E and B are perpindicular to the direction of propogation
4) E/B = c

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4
Q

is divergence cross product or dot product
is curl cross product or dot product

what is gradient using del operator

A

dot product, cross

what is gradient using del operator

The gradient is a vector field that results from the del operator acting on a scalar field

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4
Q

what did maxwell propose

what does comptons effect only depend on

A

Maxwell proposed the converse: a changing electric field has
a magnetic field associated with it.

what does comptons effect only depend on

the Compton shift, depends only on the scattering angle 0, and not
on the initial wavelength A

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5
Q

what are wave packets and what is, group velocity

A

a group of superposed waves which together form a travelling localized disturbance,

its the velocity of a representative point on the wave packet
is the rate at which the phase of the wave propagates in space. It represents the velocity at which a single point of constant phase (such as a crest or trough) moves.

group velocity is the velocity of the full packet

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6
Q

position momentum uncertainty

energy time uncertainty

uncertainty relation for circular motion

A

the position of a particle and momentum of a particle cannot be determined simultaneously with unlimited precision

energy

the energy and life of a particle in a state cannot be determined simultaneously with unlimited precision

circular motion

the angular position and angular momentum of a particle in a circular motion cannot be determined simultaneously with unlimited precision

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7
Q

what is Significance of the Poynting Vector

A

Poynting vector represents the direction and magnitude of energy flow in an electromagnetic wave

gives the rate of energy transfer per unit area for an electromagnetic wave
Its direction points along the direction in which energy propagates.

Poynting vector helps calculate the total energy flowing through a surface.

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8
Q

What the signifiance/intrpretation of wave function/Normalization of wave functions

What is borns rule

A

Probability density
The square of the absolute value of the wave function, or |ψ|2, represents the probability density of finding a particle in a specific location at a given time = 1.
Or probability of finding the particle in unit volume in
three dimensional space

Quantum state
The wave function represents the quantum state of a system, such as an atom or particle.

wave packet 𝚿 is a
probability amplitude
* The wavefunction carries information about the system

wave function is the probability amplitude

The wave function evolves according to the Schrödinger equation, which allows for the prediction of future probabilities.

BORNS RULE
The Born Rule in Quantum Mechanics is mathematically expressed as P = |ψ|²,

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9
Q

what is plane polarised, circular, eliptical,unpolorised light

A

A plane wave is called linearly polarized. horizontall
and vertically linearly polarized same phase/amplitude at a 45 degrees

If light is composed of two plane waves of equal amplitude but differing
in phase by 90°, then the light is said to be circularly polarized

If two plane waves of differing amplitude are related in phase by 90°, or
if the relative phase is other than 90° then the light is said to be
elliptically polarized

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10
Q

what is black body

A

found materials which absorb all incident rays
Such a material on heating would emit all wavelengths of radiation
absorbed

OR

bodies that have surfaces which absorb all the thermal radiation incident upon them.

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11
Q

what is classical wave theory assumption

what was the UV cathostrophe

A

Assumed that energy content of the wave is
proportional to the square of the amplitude of the waves

UV
Rayleigh and Jeans showed that the
number of modes was proportional to ν^2

also Rayleigh and Jeans considered the average energy of the
oscillators as per Maxwell-Boltzmann distribution law
as E = kBT

although the curves agree at low frequencies, classical physics predicted too much energy at high frequencies, leading to the ultraviolet catastrophe.

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12
Q

what conclusion did max plancks have regarding the average energy of the oscillators

how is energy determined for particle-particle interaction of EM radiation

A

the collection of harmonic oscillators of
different frequencies and the energy of the radiations has to be packets
of hν or nhv and thus it was related with the experimental values

particle-particle
Energy is quantized in terms of hν
Wavelength and frequency - effect on energy

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13
Q

KE of matter particles like electrons

what is the value of the compton shift h/MoC

and what is the value of h dash

A

p^2/2m

2.42410^-12
1.055
10^-34

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13
Q

In a non-dispersive medium the group velocity is equal to the phase velocity (TRUE, OR FALSE)

A

TRUE, all frequency components of a wave travel at the same speed. Therefore, the group velocity (velocity at which the wave packet or energy propagates) is equal to the phase velocity (velocity at which the phase of the wave propagates).

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14
Q

what are the formula/normalization of wave function

A

1) mathematical form = ψ Ae^i/ℏ(Px-Et)
2)intrepretation/sigificance of borns rule ψψ
3) A or finding normalization constant such that integral of - infinity to infinity ψ
ψ leads to normalization

15
Q

properties of wave function

A

ψ must be continious, single value, finite, at a single place

dψ/dx (slope) must be continous, single value and and finite

ψ must be normalizable

if ψ represents a wave packet centered at x=0 then as x = infinity ψ=0

16
Q

Explain the concept normalization

what is probability density

A

Normalization refers to the process of multiplying a wave function by a suitable
constant or adjusting its amplitude such that
integral - ∞ to + ∞ Ψ*Ψ dx =1
to ensure that the total probability of finding the particle in all possible positions is 1

prob density

Probabilty density is defined by ψ*ψ and is the probability per unit length ( for 1D case)

17
Q

what is observable

what are eigen values

what are eigen functions

what are mathematical operators

A

An observable is any physical quantity that can be measured in a quantum system, such as position, momentum, energy,

Eigen values

Eigenvalues are the possible values that can be obtained when measuring an observable. They are solutions to the eigenvalue equation:
EIGEN FUNCTIONS
An eigenfunction (or eigenstate) is a specific wavefunction that remains unchanged except for a scaling factor when acted upon by an operator representing an observable. The eigenvalue associated with the eigenfunction represents the value of the observable. operator = cap on top

MATHEMATICAL OPERATORS

Mathematical operators can be used to extract
information about the physical state in form of
observables, like momentum, particles position or energy

18
Q

what is Hamiltonian

A

The Hamiltonian is the operator corresponding to the total energy of a quantum system, which includes both kinetic and potential energies.

19
Q

a beam of free particles at incident along x-axis infinite range
and finite rane

A

No beam can go form negative infinity to postive infinity

finite range: ψ = C1e^ikx+C2e^-ikx
C2=0 as no wave is coming towards ‘-‘ x-axis

20
Q

step voltage

A

E<Vo
-∞ < x < 0
Region 1
0 < x < -0 V=Vo
C1e^ikx+C2e^-ikx

Region 2
C3e^αx+C4e^-αx
C3e^ax C4=0 no reflection

boundary:
ψI = ψII
dψI/dx
dψII/dx

C1+C2=C4
ikC1-ikC2=aC4
C2=((ik+a)/(ik-a))C1
((ik+a)/(ik-a))=1
R=1
when PE changes reflection will happen

E>Vo
-∞ < x < 0
Region 1
0 < x < -0 V=Vo
C1e^ikx+C2e^-ikx

Region 2
C3e^αx+C4e^-αx
C3e^ax C4=0 no reflection

boundary condition
x=0

ψI = ψII
dψI/dx
dψII/dx

C1+C2=C3
ikC1-ikC2=aC4
T = 4kk’/(k+k’)^2
R = ((K-K’)/(K+k’))^2
T+R=1

R=(√(2mE)/ℏ-√(2m(E-Vo)/ℏ)^2/
(√(2mE)/ℏ)-√(2m(E-Vo)/ℏ)^2 =>
(√E-√E-Vo/√E+√E-Vo)^2
=> ((1-√1-Vo/E)/
1+√1-V/E))^2
IMP!!

k1 =√(2mE)/ℏ^2
k’=√2m(E-V)/ℏ^2
E and V in joules here

L= ħ/sqrt(2m(Vo-E)) here v and e are in Joules
penetration depth for both cases

21
Q

beam of particles incident at a potential barrier

A

RI -∞ < x < 0 V=0
ψ=C1e^ikx+C2e^-ikx
RII 0 < x < a V=0
C3e^ax+C4^-ax
RIII a<x<∞ V=0
C5e^ikx+C6e^-ikx
C6=0
Boundary conditions
x=0
ψI=ψII
dψI/dx=dψII/dx
x=a
ψII=ψIII
dψII/dx=dψIII/dx

T^-1=1+[sinh]^2/
4[E/Vo][1-E/Vo] transmission coefficient
e^2κa => exponential decay
T=e^-2ka

transmission coefficient is proportional to the exponential decay factor, thus is less severe, resulting in higher transmission if mass is less.

κ = √2m(Vo-E)/h^2 here Vo-E should be in joules

22
Q

Infinite potential well, and what kind of equations are the boundary equation ISA

A

Region I -
-∞ < x < a/2
Region II
-a/2 < x < a/2
Region III
a/2 <x<∞

ψ= Acos(kx)+Bsin(kx)
boundarycondition
x=-a/2.
Acosk(a/2)-BsinK(a/2)
x=a/2
Acosk(a/2)-Bsink(a/2)
1+2=
Acosk(ka)
ψ=Bsin(kx)
ψ=o
Bsinka/2=0
sinka/2=0
ka/2 = pi,2pi,3pi
ka=2pi,4pi,6pi
quantising k
k=n*pi/ax

wave function = ψ(x)=
√2/Lcos(npi/ax)/L
=even
√2/Lsin(npi/ax)/L=odd

energy =(n^2*h^2/8ma^2)

ψI=ψII
dψI/dx=dψII/dx
ktan(ka/2)=a

ψII=ψIII
dψII/dx=dψIII/dx
kcot(ka/2)=-a
transcendental cant be solved analytically(numerically) or graphically

23
Q

finite potential well

A

Region I -
-∞ < x < a/2
Region II
-a/2 < x < a/2
Region III
a/2 <x<∞

RI= C1e^ax+C2e^-ax
C2=0
RII= C3e^ikx+C4-ikx
III=C5e^ax+C6^-ax
C5=0
ktan(ka/2)=a
PtanP=√B^2-P^2
let = √mEa^2/2ℏ^2 =P
√((mEa^a/2ℏ^2)-mEa^2/2ℏ^2))

-PcotP=√B^2-P^2
P1=√mE1a^2/2ℏ^2
P2=√mE2a^2/2ℏ^2

n^h^2/8m(a+2L)^2
n^h^2/8m(a)^2

24
Q

finite>Infite

A

finite>Infinite
k<k
p<p
E<E

25
Q

quantum oscillators

A

d^2x/dt^2+w^2x=0

V=1/2Cx^2
E=P^2/2m+V = aconst
lowest energy = 0, all Es are possible

quantum oscillators
μ=m1m2/(m1+m2)
if m1=-∞
m2=μ (which is reduced mass)

d^2x/dt^2+(C/μ)x=0
d^2ψ/dx^2+2μ/ℏ^2[E-1/2Cx^2]ψ=0
expand using power series expansion
En=(n+1/2)hv

26
Q

ISA what are features of energy, plot them, why is it possible to go to below 0k

A

energy can be quantised,
its not possible to below 0K because you can extract energy Nernst third law

27
Q

de Broglie hypothesis

question 8 derive Broglie equation

what is total transmission coefficient of individual barriers potentials

A

Moving matter (form of energy) should also exhibit wave
characteristics

Wavelengths of macro particles are extremely small to be
measured

K=1/2mv^2
in terms of v
v=√2K/m
λ=h/(m√2K/m)=
λ=h/√2Km
E=hv=1/2mv^2+P

TOTAL TRANSMISSION
the product of the barriers potentials = total coefficients