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3.1: Use the frequency of oscillation of the
electrons in the transmitting and receiving
antennae to explain the transmission and
reception of electromagnetic signals (3 Marks)
In the transmitting antenna electrons
oscillate and produce an electric field
which matches frequency of
oscillations of the e-. [1]
When an electric field of e.m. wave
encounters a receiving antenna, it
forces the e- in receiving antenna to
move, [1]
oscillating hence receiving the “signal”
wave [1]
3.1: Relate the orientation of the receiving
antenna to the plane of polarisation of
electromagnetic waves (2 Marks)
Antenna orientation matches the
plane of polarisation of the Electric
field of the e.m. wave (TV or radio) [2]
3.1: Describe what is meant by two wave sources
being in phase or out of phase. (2 Marks)
In phase: waves match with same
frequency, same displacement at
same time with path difference of zero or a
whole wavelength [1]
Out of phase: waves have same
frequency, but they are a half a
wavelength out of sync with path difference of half wavelength [1]
3.1: Explain why light from an incandescent source
is neither coherent nor monochromatic (3 Marks).
Incandescent source has charges (e-)
which are vibrating at different
frequencies and emit light waves
random directions. [1]
Range of frequencies means it is not
monochromatic [1]
and not coherent because it has dif
frequencies and they are not in
phase, there is not a constant phase
relationship [1]
3.1: Use constructive and destructive interference to explain the maximum and minimum
amplitudes (4 marks)
Constructive interference, means 2 or more waves meet when they are in phase, have
a path diff of zero or whole wavelength and a maximum amplitude wave is produced
(maxima, bright fringe). [2]
Destructive interference, means at 2 waves meet and they are out of phase, have a
path diff of half a wavelength and a minimum amplitude is produced (minima, dark
fringe). [2]
3.1: Use the principle of superposition to describe:
constructive interference, and destructive interference. (2 Marks)
If 2 waves are in phase at point on
screen, a wave crest meets crest as
path diff = mλ -> constructive
interference = MAXIMUM (a light
fringe) [1]
If 2 waves are out of phase at point
on screen, a wave crest meets trough
as path diff = (m+ ½ )λ -> destructive
interference = MINIMUM (a dark
fringe) [1]
3.1: Describe how two-slit interference is
produced in the laboratory using a coherent
light. (3 Marks)
In a lab a two-slit interference is
produced by having a coherent light
source is used [1]
two slits diffract the light which
overlaps [1]
and interferes on a screen [1]
3.1: Describe how diffraction of the light by the
slits in a two-slit interference apparatus allows
the light to overlap and hence interference (3 marks)
Diffraction is the bending of light
waves around the edges of the slits.
This spreads the light out [1]
and allows it to overlap with the
diffracted light from the other slit [1]
and hence interfere can occur. [1]
3.1: For a two-slit interference pattern, use
interference to explain the bright fringes and dark fringes (4 marks)
Bright fringes result from constructive
interference, when the path diff
between waves from the two slits = mλ , [1]
they diffract, overlap and reinforce
producing a maximum (bright fringe).
[1]
Dark fringes result from destructive
interference, when the path diff
between waves from the two slits =
(m+ ½ )λ , [1]
they diffract, overlap and annul
producing a minimum (dark fringe). [1]
3.1: Describe how diffraction by the very thin slits
in a transmission diffraction grating produces
an interference pattern. (3 Marks)
Diffraction is the bending of light
waves around the edges of the slits.
The thin slits of transmission
diffraction grating diffract the light, [1]
the light overlaps [1]
and interferes producing an
interference pattern with intense
maxima at certain angles.[1]
3.1:Describe how a transmission diffraction
grating can be used to experimentally
determine the wavelength of light from a
monochromatic source (3 Marks)
A grating can be placed at a distance
L, between a monochromatic light
source and a screen. [1]
The angle between the mth maxima
and centre of screen can be
calculated using tanθ and the
distance x between the central
maximum and mth maximum and
distance L to screen [1]
Then you can used sin θ = mλ to
determine wavelength [1]
3.1: Describe and explain the white-light pattern produced by a transmission diffraction grating,including central maxima, 1st order maxima. (5 Marks)
A central bright band is seen, it is white because path diff is zero, [1]
all wavelengths of the light constructively interfere. [1]
At m= 1 then the different wavelengths interfere constructively at different angles
causing a continuous spectrum from blue (smallest wavelength, smallest angle), to red (longest wavelength at the largest angle) [1]
Because of equation d sin θ = mλ [1]
3.2: Describe an experimental method for
investigating the relationship between the
maximum kinetic energy of the emitted
electrons, calculated from the measured
stopping voltage using and the
frequency of the light incident on a metal
surface. (3 Marks)
In an experiment incident light
/photon source shines on a
photoelectric cell, [1]
the stopping voltage which stops e-
being emitted is increased and then
measured when the e- stop being
emitted (current =0) [1]
and hence the maximum KE of e- is
calculated by EK = eV s [1]
3.2: Describe how Einstein used the concept of
photons to explain the experimental
observations of the photoelectric effect. (2 Marks)
Einstein defined a photon as a packet
of light energy E=hf [1]
And the incident photons have
energy > work function W=hf0
then the e- are emitted instantly [1]
3.2: Describe how Einstein used the concept of
the conservation of energy to explain the
experimental observations of the
photoelectric effect. (3 Marks)
Photon has energy E=hf [1]
He used the conservation of energy to
explain that 1 photon gives 1 electron
all its energy. [1]
Ek max = hf − W [1]
3.2: Describe the purpose of the following features of a simple X-ray tube: Filament, Target, Potential difference across tube, Evacuated tube, Means of Cooling Target (List: 5 marks)
Filament: emits electrons
Target: Where electrons collide with target Atoms to produce X-Rays
Potential difference across tube: accelerates electrons to high speeds (KE)
Evacuated Tube: ensures that there are no other molecules to collide and reduce KE of
electrons
Means of Cooling Target: Reduce heat of target
3.2: Describe the energy changes that occur
during the production of X-rays, including the
heat produced. ( 4 marks)
The large potential difference (W=qΔV)
accelerates electrons so they gain KE
[1]
As the e- hit the target atoms and
pass through the spaces in the atoms
they lose KE [1] converting their
energy into X-ray photons [1]
Or KE lost is converted into heat. [1]
3.2: Explain the continuous range of frequencies
and the maximum frequency in the spectrum
of the X-rays. (5 Marks)
The continuous range of frequencies
of X-rays is due to the e- being slowed
down as it passes through the target
metal and is attracted to +ve nuclei,
[1]
it loses KE converted into X-ray
photon, by conservation of energy. [1]
Closeness of electrons path to nuclei
affects the amount of KE lost, [1]
producing the range of diff energy X-
rays.[1]
The maximum frequency (fmax) is due
to the e- hitting a nucleus and losing
all its KE energy and producing a
maximum energy photon, by
conservation of energy. [1]
3.2: Explain the effect of manipulating the
potential difference across the X-ray tube on
an X-ray spectrum. (3 Marks)
The potential difference effects the
kinetic energy given to the electrons
W=qΔV [1]
and hence the energy and frequency
E=hf of the X-rays produced. [1]
Increase potential difference,
increases KE of e-, increases the
energy and frequency of X-ray
photons, and hence increases fmax.
3.2: Explain the effect of manipulating the filament
current in the X-ray tube on an X-ray spectrum. (3 Marks)
Manipulating the filament current
effects the number of electrons
emitted [1]
and hence the number of X-rays
produced, hence the intensity of the X-
rays. [1]
This decreases the time/ exposure
time needed to take an X-ray image
in. [1]
3.2: Explain the effect of the filament current on
the intensity of X-rays produced by an X-ray
tube (3 Marks)
Manipulating the filament current
effects the number of electrons
emitted [1]
and hence the number of X-rays
produced, hence the intensity of the X-
rays. [1]
Increase current, increases number of
e-, increases number of X-ray
photons. [1]
3.2: Relate the penetrating power (hardness) of X-
rays required to pass through a particular
type of material to the energy and frequency
of the X-rays. (3 Marks)
Accelerating voltages adjusts the
penetrating power/ hardness of X-
rays [1]'
Higher density/ atomic number/
thicker materials require higher
voltage [1]
to produce higher penetrating power/
higher energy X-rays [1]
3.2: Relate the attenuation of X-rays to the types
of tissue through which they pass. (4 Marks)
Attenuation = absorption of X-rays by
materials [1]
High density like bones results in high
attenuation [1]
Areas of high attenuation appear
whiter, because they absorb more X-
rays and don’t hit the film [1]
High atomic number results in high
attenuation
Thicker results like large chest in high
attenuation. [1]
3.2: Relate the minimum exposure time for X‑ray
photographs of a given hardness to the
intensity of the X-rays. (3 Marks)
The minimum exposure time is
controlled by the current in filament.
[1]
A higher current produces more e-
which produces more X-rays =higher
intensity of X-rays [1]
Higher current can reduce the
exposure time [1]
3.2: Describe two-slit interference pattern
produced by electrons in double-slit
experiments. (3 Marks)
The 2-slit interference pattern
produced by e- at a certain speed
proves that e- have wave properties.
[1]
Two slits diffract electrons, they then
overlap produce an interference
pattern [1]
The similar interference pattern
produced is e- have same wavelength
as the light (e.m. wave) used. [1]
3.2: Describe the Davisson–Germer experiment, in
which the diffraction of electrons by the
surface layers of a crystal lattice was observed. (3 Marks)
In the Davisson Germer experiment
e- strike crystal (nickel) [1]
and this acts as a diffraction grating
as spacing between the crystal
structure d [1]
is similar size to the wavelength of e-
[1]
3.2: Compare the de Broglie wavelength of
electrons with the wavelength required to
produce the observations of the Davisson–
Germer experiment and in two-slit
interference experiments. (3 Marks)
the wavelength of electron must be
the same as the light waves [1]
to diffract, overlap and produce
interference pattern [1]
Davisson-Germer the crystal acts like
a diffraction grating as d is similar size
to electron wavelength. [1]
3.3: Describe the changes in the spectrum of an
incandescent source as the temperature of
the incandescent source increases. (3 Marks)
As temperature increases, the spectrum shifts from red to blue region of visible spectrum [2]
(graph curve shifts to the left i.e. to lower wavelength)
Also, the intensity increases as the temperature increases [1] (graph shifts up)
3.3: Describe the general characteristics of the line
emission spectra of elements. (2 Marks)
Line emission spectrum is black [1] with discrete coloured lines (λ) [1]
3.3: Explain how the uniqueness of the spectra of
elements can be used to identify the presence
of an element. (3 Marks)
Each element when excited emits a unique spectrum [1].
So comparing the observed spectrum with known spectrum [1] and by matching all the wavelength lines [1] you can identify the element present.
3.3: Explain the production of characteristic X-rays
in an X-ray tube. (3 Marks)
In an X-ray tube, incident e- collide with the lower energy inner shell e- of the target atoms. [1]
This excites the e- into a higher energy level, and then falls back down [1] and converts energy by emitting extra X-ray photons causing the characteristic peaks at certain frequencies [1]
3.3: Explain how the presence of discrete
frequencies in line emission spectra provides
evidence for the existence of states with
discrete electron energy‑levels in atoms. (3 Marks)
Excited atoms emit line emission spectrum as the atoms de-excite, returning to lower state [1].
The energy transition releases a photon matching the energy difference (ΔE between energy levels) . [1]
The frequency of the photon found by E=hf, is discrete, providing evidence that there are energy levels/shells in atoms. [1]
3.3: Explain why there are no absorption lines in
the visible region for hydrogen at room
temperature. ( 3 Marks)
At room temperature hydrogen is in
ground state, [1] and can only absorb photons from UV
region, therefore visible light cannot excite the 1 electron from ground state to n=1, or n=1 to n=2. [1]
this means the absorption line is not in visible region [1]
3.3: Account for the presence of absorption lines
(Fraunhofer lines) in the Sun’s spectrum. (3 Marks)
The cooler outer gaseous layers of the Sun (corona) absorbs photons produced by the sun’s core [1].
These photons match energy level transitions in atoms as ΔE=hf [1]
This excites the atoms in the corona. These electrons then fall back and emit photons in random directions [1], resulting in the dark absorption lines in the Sun’s spectrum , which are the Fraunhofer lines.
![<p><strong>3.3: </strong>Using electron energy levels for lithium (image</p><p>shown on right), analyse and explain the:</p><p>characteristic wavelengths and line spectra, and fluorescence. [4 Marks]</p>](https://assets.knowt.com/user-attachments/c147adc3-dcd2-412d-81ff-21b4ef5ef08d.png)
3.3: Using electron energy levels for lithium (image
shown on right), analyse and explain the:
characteristic wavelengths and line spectra, and fluorescence. [4 Marks]
Characteristic wavelengths result from electron transitions [1] between energy levels ΔE=hf [1]
Fluorescence is the process of an atom absorbing a high energy photon (UV) [1] - purple arrow up on diagram
Atom falls back down via multiple transitions producing
many lower energy photons (visible) [1] - red arrows down on diagram.
3.3: Compare the process of stimulated emission
with that of ordinary (or spontaneous)
emission. [5 Marks]
Spontaneous emission: Incident photon=energy gap in atom △E=hf, triggering atom to absorb photon, atom becomes excited, [1] and transits to lower energy level then emits photon at the same frequency/ energy [1].
Stimulated emission: e- already in excited state, [1] incident photon matches energy gap △E=hf, and stimulates the electron to deexcite, [1] emitting two identical photons in phase
3.3: Explain how stimulated emission can produce
coherent light in a laser. [3 Marks]
Incident photon has same energy as gap in atom, (ΔE=hf) [1], forces stimulated emission by triggering the excited e- to deexcite and emit a photon which is coherent with incident photon, resulting 2 photons in phase and coherent= laser. [2]
3.3: Explain the conditions required for stimulated
emission to predominate over absorption
when light is incident on a set of atoms. [3 Marks]
1) Electron/atom needs to be in an excited, metastable state
2) Incident photon has energy = ΔE energy gap of atom
3) Population inversion, so more e- in an excited state than in lower state.
4) Stimulated emissions>absorbtion
[any 3]
3.3: Describe two useful properties of laser light. [2 Marks]
Coherent, Monochromatic, high intensity, unidirectional (Choose any 2)
3.3: State two requirements for the safe handling
of lasers. [ 2 Marks]
Do not shine in eyes, use lasar goggles
3.4: Describe the electromagnetic, weak nuclear, and strong nuclear forces in terms of
gauge bosons.
Identify which types of fundamental particles are affected by each type of fundamental
force. (6 Marks)
Electromagnetic:
Force + Gauge Bosons:
2 e- (charged particles) repelling, photon (gauge boson) emitted by 1 particle
causes recoil as transfers photon momentum and energy to other e- (charged particle)
Type of Fundamental particles involved:
electrons, muons, tau particles(protons)
Weak nuclear:
Force + Gauge Bosons:
neutrinos interact exchange W/ Z bosons
Type of Fundamental particles involved:
neutrinos
Strong nuclear:
Force + Gauge Bosons:
nucleons (neutrons protons) in nucleus held together, nucleons exchange mesons (like pions), gluons (gauge boson) exchange between mesons/ pions mediate the force
Type of Fundamental particles involved:
mesons, nucleons or baryons
(i.e. hadrons)
3.4: Describe the properties of an antimatter particle. (Charge + Mass) 2 Marks
antimatter have opposite charge [1], same mass [1]
3.4: Describe how protons and neutrons (or other
baryons) can be formed from different
combinations of quarks. (4 Marks)
All baryons have 3 quarks [1]
e.g. proton, neutron
Proton has 2 up and 1 down quarks
(u,u,d) = +1e charge [1]
Neutron has 1 up and 2 down quarks
(u,d,d) = 0 charge [1]
Antibaryons have 3 antiquarks
3.4: Describe how pions and other mesons consist
of different combinations of quarks and
antiquarks. (3 Marks).
Pions and mesons have a 2 quark composition [1], being 1 quark and 1 antiquark [1]
Pion,π+ (pion plus) has 1 up and 1 anti-down quark = +1e charge [1]