Physics particles

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82 Terms

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Atomic radius

1x10-10m

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Nuclear radius

1x10-15m

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Nucleon number

number of protons plus the number of neutrons in an atom

  • Always a whole number

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Isotopes

elements with the same number of protons and electrons, but a different number

of neutrons.

  • Same charge as each other

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Radioisotope

radioactive isotope of an element

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Ions

different charges to their equivalent atom (electron gained or lost)

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Four fundamental forces

  • Strong nuclear

  • Weak nuclear

  • Electromagnetic

  • Gravity

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Strong Nuclear force

  • Both attractive and repulsive

  • Attractive over short-range (up to 3 fm)

  • Repulsive over very short range (under 0.5 fm)

  • Prevents electromagnetic repulsive forces between protons causing nucleus to fly apart

<ul><li><p><span style="background-color: transparent;"><span>Both attractive and repulsive</span></span></p></li><li><p><span style="background-color: transparent;"><span>Attractive over short-range (up to 3 fm)</span></span></p></li><li><p><span style="background-color: transparent;"><span>Repulsive over very short range (under 0.5 fm)</span></span></p></li><li><p><span style="background-color: transparent;"><span>Prevents electromagnetic repulsive forces between protons causing nucleus to fly apart</span></span></p></li></ul><p></p>
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Unstable nucleus

nucleus that will change (by undergoing fission, fusion or emitting radiation)

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electron anti-neutrino

by product of beta decay

  • fundamental, nearly massless particles

  • Second most common particle in the universe


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Specific charge [C]

the relative charge of a particle divided by its mass (the ratio of its total charge to its mass)

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Antiparticles

subatomic particles that have the same mass as their corresponding matter particle but with the opposite electric charge

  • An antiparticle has the exact same mass as its corresponding particle.

  • The electric charge is opposite to the particle

  • Have opposite spin and colour (for quarks)

  • often denoted with a bar over their symbol or a different symbol

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Annihilation

when a particle and the corresponding antiparticle meet and their mass is converted into radiation energy.

  • This process releases 2 photons (a single photon cannot ensure a total momentum of 0 after the collision)

  • The minimum energy of each photon, hfmin ,is given by equating the energy of the two photons, 2hfmin, to the rest energy of the particle and antiparticle

  • I.e. 2hfmin = 2E0, where E0 is the rest energy of the particle

  • Minimum energy of each photon produced hfmin = E0

  • Usually gamma-ray photon produced

<p>when a particle and the corresponding antiparticle meet and their mass is converted into radiation energy.</p><ul><li><p>This process releases 2 photons (a single photon cannot ensure a total momentum of 0 after the collision)</p></li><li><p>The minimum energy of each photon, hf<sub>min</sub> ,is given by equating the energy of the two photons, 2hf<sub>min</sub>, to the rest energy of the particle and antiparticle</p></li><li><p>I.e. 2hf<sub><sup>min</sup></sub> = 2E0, where E0 is the rest energy of the particle</p></li><li><p>Minimum energy of each photon produced hf<sub>min</sub> = E<sub>0</sub></p></li><li><p>Usually gamma-ray photon produced</p></li></ul><p></p>
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Pair production

when a photon creates a particle and the corresponding antiparticle, and vanishes in the process

  • For a particle and antiparticle, with both rest energy E0, you can calculate the minimum energy hfmin and minimum frequency Fmin that the photon must have to produce the particle-antiparticle pair

  • Minimum energy of photon needed = hfmin = 2E0

  • Starts with a gamma photon, and branches out to produce a particle and anti-particle, nearly always a electron and a positron

<p>when a photon creates a particle and the corresponding antiparticle, and vanishes in the process</p><ul><li><p>For a particle and antiparticle, with both rest energy E0, you can calculate the minimum energy hf<sub>min</sub> and minimum frequency F<sub>min</sub> that the photon must have to produce the particle-antiparticle pair</p></li><li><p>Minimum energy of photon needed = hf<sub>min</sub> = 2E<sub>0</sub></p></li><li><p>Starts with a gamma photon, and branches out to produce a particle and anti-particle, nearly always a electron and a positron </p></li></ul><p></p>
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Nucleon

a proton or neutron in the nucleus

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Nuclide

each type of nucleus

  • Labelled using isotope notation

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Strong nuclear force

a force that holds a nucleus together and overcomes the electrostatic force of repulsion between the protons in the nucleus, keeping the protons and neutrons together

  • Same effect between two protons as it does between two neutrons or a proton and a neutron

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Strong nuclear force effect

Attraction from around 3fm to 0.5 fm, less than 0.5 fm it is a repulsive force

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Beta decay

when a neutron in the nucleus changes into a proton

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Neutrinos

subatomic particles which carries some energy away from the nucleus during beta decay

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Antimatter

the counterpart to ordinary matter, consisting of particles with the same mass but opposite charge

  • When antimatter and matter particles meet they destroy each other and radiation is released

  • Can make use of this in a positron emitting tomography (PET) hospital scanner

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positron

antiparticle of the electron

<p>antiparticle of the electron</p>
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Positron emission

takes place when a proton changes to a neutron in an unstable nucleus with too many protons

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PET Scanner used for brain scan

  • Positron emitting isotope administered to patient and some reaches brain via blood

  • Each positron emitted travels no further than a few millimeters before it meets electron and annihilate each other, causing two gamma photons to be produced and are sensed by detectors

  • This builds up an image in a computer and an image is built up from the detector signal of where the positron emitting nuclei are inside the brain

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Rest energy

mass of a particle when it is stationary

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Dirac’s theory of antiparticles

  • Annihilates the particle and itself if they meet, converting total mass into photons

  • Has exactly the same rest mass as particle

  • Has exactly opposite charge to particle if particle has a charge

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Millions of electron volts [MeV]

Energy of a particle / Antiparticle unit

  • 1MeV = 1.6 x10-13J

  • Defined as the energy transferred when an electron is moved through a potential difference of 1 volt

  • Can be calculated using E=mc2

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Minimum energy of each photon produced equation

min = E0

  • min being minimum energy of each photon produced

  • E0 being rest energy

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Minimum energy of each photon needed equation

min = 2E0

  • min being minimum energy of each photon needed

  • E0 being rest energy

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Exchange particles

particles that exist temporarily to cause ‘particle interactions’

e.g.

  • electrostatic attraction/repulstion

  • ß- decay

  • Electromagnetic force: exchange particles = photon

  • Weak nuclear force exchange: exchange particles = W+, W-, Z+

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Feynman diagram

represents particle interactions

  • Charge must be conserved at each vertex

<p>represents particle interactions</p><ul><li><p>Charge must be conserved at each vertex</p></li></ul><p></p>
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W bosons and Z bosons

name of the exchange particle for a weak nuclear force

  • Non-zero rest mass

  • Very short range (no more than 0.001 fm)

  • Positively or negatively charged (W+ or W-)

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Quarks

make up particles like protons and neutrons

  • Twelve quarks

  • 6 particles, 6 anti-partiles

  • Negative name particles are negatively charged

  • Does interact via / experience a strong nuclear force

  • Fractional charged

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Fundamental particles

particles which cannot be broken down into smaller particles

  • E.g. neutrinos, anti-neutrino, electrons, positrons, leptons, tau, quarks

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Protons quark structure

made up from 3 quarks (2 up quarks and 1 down quark )

  • p = u + u + d

<p>made up from 3 quarks (2 up quarks and 1 down quark )</p><ul><li><p>p = u + u + d</p></li></ul><p></p>
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Neutron quark structure

made up from 3 quarks (2 down quarks and 1 up quark)

  • n = u + d + d

<p>made up from 3 quarks (2 down quarks and 1 up quark)</p><ul><li><p>n = u + d + d</p></li></ul><p></p>
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Leptons

  • Twelve leptons

  • Six particles, six antiparticles

  • Don’t interact via / experience a strong nuclear force

  • Have integer charge

  • Lighter than hadrons

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List of particle Leptons

  • Electron

  • Electron Neutrino

  • Muon

  • Muon Neutrino

  • Tau 

  • Tau Neutrino

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List of antiparticle Leptons

  • Positron

  • Electron anti-neutrino

  • Anti-muon

  • Muon anti-neutrino

  • Anti-tau

  • Tau anti-neutrino

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List of particle Quarks

  • Up

  • Down

  • Top

  • Bottom

  • Strange

  • Charm

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List of particle anti-quarks

  • Anti- Up

  • Anti - Down

  • Anti - Top

  • Anti - Bottom

  • Anti - Strange

  • Anti - Charm

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Hadrons

  • Heavy

  • Not fundamental particles

  • Subject to the strong interaction

  • Two types:

    • Baryons

    • Mesons

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Baryons

  • made of 3 quarks

  • Protons are the only stable baryon which other baryons eventually decay to

  • E.g protons and neutrons

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Mesons

made of 1 quark and 1 anti-quark

  • E.g pions and kaons

    • Kaons - have to have a strange or anti-strange quark

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Quantum numbers

numbers that must be conserved in particle interactions (value before an interaction = value after interaction)

  • Charge

  • Mass-energy

  • Hadron number

  • Baryon number

  • Strangeness

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Baryon number

  • Baryon Number = 1 (e.g. proton)

  • Anti-Baryon = -1 (e.g. anti-proton)

  • Baryon number of quark = ⅓

  • Baryon number of anti-quark = -⅓

  • Non-baryon = 0 (e.g. electron)

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Lepton number

  • Lepton number = 1

  • Anti-lepton number = -1

  • Lepton number of quark and anti-quark = 0

  • Non-lepton = 0 (anything else)

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Strangeness

  • Strange quark = -1

  • Anti-strange quark = 1

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Hadrons

  • Pion - another exchange particle of the strong nuclear force, between proton (p+) and neutron (n0)

    • Kaons can decay to pions

  • Gluons - holds together the quarks within hadrons such as protons and neutrons

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General information about particles

  • Particles beginning with ‘p’ are the most stable

  • Many exist for very short periods of time due to being unstable

  • Decay is a weak interaction

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Strange quarks

  • Strange quarks produce via strong nuclear interactions

  • Created in pairs

  • Strangeness conserved in the strong interactions

  • Can change by 0, +1, -1 in weak interactions

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Lepton decay

  • Taus decay into muons

  • Muons decay into electrons

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Electromagnetic waves

consists of an electric wave and a magnetic wave, which travel together and vibrate

  • Travel and vibrate at right angles to each other and to the direction in which they are travelling

  • Travel and vibrate in phase with each other

  • Emitted as short bursts of waves, with each burst leaving the source in a different direction

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Photons

a packet of electromagnetic waves that are emitted by a charged particle when it loses energy

  • Happens when a fast moving electron is stopped, slows down or changes direction

  • Happens when an electron in a shell of an atoms moves to a different shell of lower energy

  • Established by Einstein when he used his ideas to explain the photoelectric effect

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Photon energy equation

E = hf

  • h as plancks constant

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Laser beams

consists of photons of the same frequency

  • Power of laser beam is the energy pers second transferred by photons

  • Laser beam power equation: power of beam = nhf

  • n = number of photons in beam passing a fixed point per second

  • hf = energy in each photon

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Nature of light

Light sometimes behaves like a particle

Particles of light are called photons and have zero rest mass

Can be:

  • reflected

  • refracted

  • diffracted

  • Interference

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Planck’s constant

 6.63 x 10-34 Js

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Electron volt (eV)

the amount of energy gained by an electron as it accelerates through a potential difference of 1 volt

  • an alternative unit to the joule for energy

  • 1eV = 1.6 x 10-19J

  • 1eV has the same magnitude as the charge of single electron

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Photon emissions

  • Emitted when an electron (in an atom) moves from a high energy level to a low energy level

  • Energy it loses is emitted as a photon

  • Can also be atoms in a sample going from high energy level to a low energy level

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Energy levels diagram

  • Negative value imply it is bound to something

  • Photons lose energy to move to a lower energy level (if the levels were given positive values, they would be gaining energy)

  • Must have 0 energy when they are far away from the nucleus (no longer bound to the atom at this highest 0eV energy level)

<ul><li><p><span style="background-color: transparent;"><span>Negative value imply it is bound to something</span></span></p></li><li><p><span style="background-color: transparent;"><span>Photons lose energy to move to a lower energy level (if the levels were given positive values, they would be gaining energy)</span></span></p></li><li><p><span style="background-color: transparent;"><span>Must have 0 energy when they are far away from the nucleus (no longer bound to the atom at this highest 0eV energy level)</span></span></p></li></ul><p></p>
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Range of wavelength for visible light

400nm to 700nm

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Photon emission

  • Electrons becom excited (gain energy when the gas is heated to a high temperature)

  • emitted when an electron (in an atom) moves from a higher energy level to a lower energy level. 

  • The energy that it loses is emitted as a photon

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Two types of atomic line spectra

  • Emission spectra

  • Absorption spectra

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Emission spectra

certain wavelengths / colours of light are given out / emitted

  • Appears as bright coloured lines on a dark background

  • Can be produced by heating a gas

  • Certain wavelengths (colours) of light will be emitted

<p>certain wavelengths / colours of light are given out / emitted </p><ul><li><p>Appears as bright coloured lines on a dark background</p></li><li><p>Can be produced by heating a gas</p></li><li><p>Certain wavelengths (colours) of light will be emitted</p></li></ul><p></p>
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Absorption spectra

certain wavelength / colours of light are taken in / absorbed.

  • Will appear as dark lines on a spectrum when viewed with a spectrometer

  • Can be produced by shining light through a sample of an element (normally as a gas) and observing the wavelengths that have been absorbed

<p>certain wavelength / colours of light are taken in / absorbed.</p><ul><li><p>Will appear as dark lines on a spectrum when viewed with a spectrometer </p></li><li><p>Can be produced by shining light through a sample of an element (normally as a gas) and observing the wavelengths that have been absorbed</p></li></ul><p></p>
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Energy levels

quantised places for electrons(electron shells)

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Ionisation

when the electron moves to 0eV energy level , the electron is no longer bound to the atom (leaving the atom)

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Photoelectric effect

process of electrons being emitted from a material

  • When a photon is absorbed by an electron it will excite the electron to a higher energy level

  • If the energy of an incoming photon is big enough, then the electron will escape the atom and the atom is now ionised

  • It is evidence of the particle theory of light

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Photoelectric effect Process

  • Ultraviolet light photons excite electrons in the zinc / ionise the zinc

  • Electrons leave the zinc plate making it positively charged

  • Electrons from the bass rod are attracted towards the zinc

  • Leaves brass rod with a positive charge at the bottom

  • Which attracts the negatively charged gold leaf

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Work function

the minimum energy needed to ionise a material

  • Usually defined from the ground state

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Threshold frequency

the minimum frequency associated with the work function energy, if a photon has a lower frequency than the threshold frequency then it cannot ionise the atom

  • When over threshold frequency, the extra energy becomes kinetic energy of the photoelectron

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Photoelectric effect equations

ɸ = hft

  • h - planck’s constant [Js]

  • ft - the threshold frequency [Hz]

  • ɸ (phi) - the work function [J]

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Conservation of energy equation

hf = ɸ + Ek max

  • hf - the energy of an incident photon [J]

  • ɸ (phi) - the work function [J]

  • Ek max - the maximum kinetic energy of the emitted electron

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higher intensity light on photoelectric effect

  • More intense light hitting a metal, more photons per second hit the metal

  • More photoelectrons emitted per second

  • No change to velocity or kinetic energy of electrons

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Higher frequency light on hitting a metal (shorter wavelength)

  • Each photon has more energy (coming in)

  • Each emitted photoelectron has greater kinetic energy

  • No effect on number of electron emitted per second

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Stopping potential

the minimum potential required to stop photoelectric emission

  • Depends on the metal, intensity and frequency of incident light

  • Kinetic energy of electrons is zero because extra work needs to be done against the potential difference 

  • Kinetic energy maximum of emitted electrons = electronic charge x velocity

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Wave-particle duality

light sometimes behaves as a wave and sometimes as a particle

  • Particles only display wave properties only when they are small and relatilistic (moving at a significant proportion to speed of light)

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Particle properties of light

  • Photoelectric effect

  • Line spectra

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Louis de Broglie discovery

said that when a particle has momentum it has a corresponding wavelength

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Formula for de Broglie wavelength

λdb = h / p or λdb = h / mv

  • λdb - de Broglie wavelength (of a particle)

  • h - planck’s constant

  • p or mv - the momentum

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Wave properties of light

  • Reflection

  • Refraction

  • Diffraction 

  • Interference

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