Quantum Physics 9702

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33 Terms

1
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Photoelectric equation

E= hf = φ + KE_max (0.5mv^2 max)

- E = hf, is energy of a photon which is transferred to an electron to release it from a material.

- f= frequency of incident photons

- φ = work function J

<p>E= hf = φ + KE_max (0.5mv^2 max)</p><p>- E = hf, is energy of a photon which is transferred to an electron to release it from a material.</p><p>- f= frequency of incident photons</p><p>- φ = work function J</p>
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Energy at maximum k.e. = hf - φ (graph)

- Energy at maximum k.e. = hf - φ

- work function = h * threshold frequency

- The work function Φ is the y-intercept.

- The threshold frequency f0 is the x-intercept.

- The gradient is equal to Planck's constant h

- There are no electrons emitted below the threshold frequency f0

<p>- Energy at maximum k.e. = hf - φ</p><p>- work function = h * threshold frequency</p><p>- The work function Φ is the y-intercept.</p><p>- The threshold frequency f0 is the x-intercept.</p><p>- The gradient is equal to Planck's constant h</p><p>- There are no electrons emitted below the threshold frequency f0</p>
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Photoelectric current relation to intensity

- Proportional

- Increasing intensity = increasing no. of photons striking metal

- Increases no. of photoelectrons emitted, as each photoelectron absorbs on photon

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Wave-particle duality

Light/EM radiation can behave like particles (photons) and waves.

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Evidence for particulate nature of EM radiation

Photoelectric effect.

- electron needs a minimum energy to escape, and energy is absorbed in packets related to frequency

- minimum threshold frequency required to escape

- each electron absorbs only one whole packet of energy, unrelated to the number of packets

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Evidence for wave nature of EM radiation

Diffraction and interference.

- Both purely wave properties that EM radiation exhibits through electron diffraction

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de Broglie wavelength

The wavelength associated with a moving particle.

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de Broglie wavelength of a particle equation

λ = h/p = h/mv

- p is momentum of the particle

<p>λ = h/p = h/mv</p><p>- p is momentum of the particle</p>
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de Broglie wavelength of a particle related to kinetic energy equation

- so E= p^2/2m

- so p= (2mE)^0.5

- so λ= h/(2mE)^0.5

<p>- so E= p^2/2m</p><p>- so p= (2mE)^0.5</p><p>- so λ= h/(2mE)^0.5</p>
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Electron energy levels

The only certain energies that an electron can have.

- Usually they occupy the lowest (ground) level

- gain energy by collisions/absorbing photons/heat

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Excitation

When electrons move up an energy level.

- they're in an excited state

- enough energy to be removed from atom: ionisation

- returns to lower energy state: releases energy as a photon

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Line spectra

When excited atoms emit light of certain wavelengths which correspond to certain colours.

- Each element produces a unique set of spectrum lines.

<p>When excited atoms emit light of certain wavelengths which correspond to certain colours.</p><p>- Each element produces a unique set of spectrum lines.</p>
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Two types of line spectra

Emission spectra and absorption spectra

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Emission spectra

- emission spectrum consists of discrete wavelengths (which are different colours)

- Electron transfers higher to lower energy level: emission of photon, which has a wavelength that corresponds to the discrete energy change

- each transition is a different wavelength of light = 1 line in the spectrum

ΔE = hf or hc/λ

<p>- emission spectrum consists of discrete wavelengths (which are different colours)</p><p>- Electron transfers higher to lower energy level: emission of photon, which has a wavelength that corresponds to the discrete energy change</p><p>- each transition is a different wavelength of light = 1 line in the spectrum</p><p>ΔE = hf or hc/λ</p>
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Emission spectra is evidence that

Electrons in atoms can only transition between discrete energy levels.

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Absorption spectra

- An atom is raised to excited state through absorption of a photon

- consists of a continuous spectrum with dark lines at certain wavelengths which represent different energy levels of the atom

- when electrons return to lower levels, photons are emitted in all directions, so some wavelengths appear to be missing

<p>- An atom is raised to excited state through absorption of a photon</p><p>- consists of a continuous spectrum with dark lines at certain wavelengths which represent different energy levels of the atom</p><p>- when electrons return to lower levels, photons are emitted in all directions, so some wavelengths appear to be missing</p>
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Emission and absorption spectra

The wavelengths missing from an absorption spectrum are the same as their corresponding emission spectra of the same element.

<p>The wavelengths missing from an absorption spectrum are the same as their corresponding emission spectra of the same element.</p>
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Calculating discrete energies

- The difference between two energy levels= energy of a specific photon

ΔE = hf = E2 - E1

- E1 = energy of lower level and E2= energy of the higher level

and

ΔE = hc/λ = E2 - E1

so λ= hc/(E2-E1)

so λ and energy change are inversely proportional

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Photon

A quantum of energy of electromagnetic radiation.

(Fundamental particles that make up electromagnetic radiation. Light is quantised, or carried in discrete packets)

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Therefore energy of photon is proportional to

- Directly proportional to frequency of electromagnetic radiation

- Inversely proportional to wavelength of electromagnetic radiation

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Photon momentum

p = E/c

- p = momentum of photon

- E = energy of photon

- c = speed of light

(has no mass but has momentum)

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Electronvolt (eV)

= energy gained by an electron travelling, from rest, through a potential difference of one volt

- Unit of energy.

- Derived from E = Q/V (which is from P = IV)

<p>= energy gained by an electron travelling, from rest, through a potential difference of one volt</p><p>- Unit of energy.</p><p>- Derived from E = Q/V (which is from P = IV)</p>
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Relation to kinetic energy

- If an electron accelerates from rest, an electronvolt is equal to the kinetic energy gained:

eV = ½ mv2

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Photoelectric effect

- Electrons are emitted from the surface of a metal upon the absorption of electromagnetic radiation.

- Removed electrons are photoelectrons

- Each electron absorbs one photon.

<p>- Electrons are emitted from the surface of a metal upon the absorption of electromagnetic radiation.</p><p>- Removed electrons are photoelectrons</p><p>- Each electron absorbs one photon.</p>
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Threshold frequency (property of a metal)

- The minimum frequency of incident electromagnetic radiation required to remove a photoelectron from the surface of a metal.

(Only the frequencies of light above a threshold frequency will emit a photoelectron)

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Threshold wavelength (property of a metal)

The longest wavelength of incident electromagnetic radiation that would remove a photoelectron from the surface of a metal

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φ Work function/threshold energy (Property of a metal)

The minimum energy required to remove a photoelectron from the surface of a metal.

- One electron absorbs one photon, so to escape the surface of a metal, an electron must absorb energy ≥ φ.

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Photoelectric equation demonstrates...

- If the frequency of incident photons are too low, and energy isn't enough to overcome the work function (φ), electrons won't emit

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Intensity of EM radiation

Proportional to number of photons striking/incident on the surface of the metal.

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Maximum kinetic energy & incident intensity of EM radiation

- Max k.e. is independent of incident intensity

- Each electron can only absorb one photon,

- k.e. is dependent on the frequency of radiation

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Photoelectric current

Number of photoelectrons emitted per second.

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Electromagnetic radiation nature

Particulate nature. Made up of particles.

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Photon energy formula

E = hf or hc/λ

- E = energy of photon / J

- h = Planck's constant (J s)

- f = frequency Hertz/Hz

- c = speed of light (m s^-1)

- λ = wavelength (m)

<p>E = hf or hc/λ</p><p>- E = energy of photon / J</p><p>- h = Planck's constant (J s)</p><p>- f = frequency Hertz/Hz</p><p>- c = speed of light (m s^-1)</p><p>- λ = wavelength (m)</p>