MODULE 7 IQ3 Flashcards

You may prefer our related Brainscape-certified flashcards:
1
Q

what are blackbodies

A

emits EMR over a wide range of wavelengths
- the dominant wavelengths of an object will largely depends on its surface temperature
- idealistic object that absorbs all EMR that is incident on it –> purely theoretical
- because they absorb all EMR, they absorb all wavelengths –> produces a continuous spectrum

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

what is blackbody radiation

A
  • at a specific temperature, the relative intensities and wavelengths emitted by the blackbody changes
  • each temperature has a corresponding peak intensity, and the wavelength at which this occurs is the dominant/peak wavelength
  • as we move past the peak wavelength, a longer wavelength corresponds to a lower intensity
  • the cooler the star is, the longer the wavelength of the dominant colour is
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

wein’s law theory

A

the higher the surface temperature of the object, the shorter the dominant wavelength is
- thus by determining a star’s dominant wavelength, we can approximate its surface temperature in Kelvin

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

wein’s law formula

A

λ = b/T

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

UV catastrophe

A

known problem of black body radiation
- classical model for BBR is the Rayleigh-Jean’s Law and is based on thermodynamics alongside the classical model of light
- model agrees with experimental data for longer wavelengths of BBR, however there is a fatal discrepancy at shorter lengths –> the model predicts infinite intensity of radiation emission when the peak wavelength is int he ultraviolet range
- violates law of conservation of energy

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

planck’s solution to the UV catastrophe

A

suggested that blackbodies were cavaties that caused specific frequency atomic oscillations, and that radiation that emitted from these oscillations would have a discrete value of energy
- thus, when blackbody emits or absorbs radiation, it has to be an integer multiple of this quantised value, and if it was not, it would not be absorbed or emitted

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

planck’s solution equation

A

E = nhf
h = 6.626 x 10^-31 Js

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

continuous spectrum?

A

a black body with thermal equilibrium will emit EMR in quantised values
- distinction between wavelengths emitted by black bodies are so small that it appears to be a continuous spectrum

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

are stars approximate black bodies

A

stars are treated as approximate black bodies, since they mainly emit reflected EMR
- because stars have high pressures and temperatures, produce a continuous spectrum

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

what is the photoelectric effect

A

phenomenon when electrons are released from a metal’s surface when light is incident upon it

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

hertz’s observations on the photoelectric effect

A

observed that higher frequency EMR would induce stronger sparking
- if he used glass to filter out UV light, the lower frequency EMR could not produce sparking even if he increased its intensity
- when quartz is used to filter out lower-frequency EMR, sparks could be produced, and the higher the intensity of the UV light, the higher the intensity of the sparking
- these observations conflict with maxwell’s wave theory which says that the energy of a wave is related to its intensity or frequency

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

what are cathode ray tubes

A
  • electrons at the cathode, in a cathode ray tube are ‘boiled off’
  • these electrons move towards a positive anode, converting electrical energy into KE
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

photoelectric effect in cathode ray tubes

A
  • for each metal surface, electron emission only occurred if the frequency of incident light exceeded a certain threshold
  • if photoemission occurred, increasing the intensity of light only increased the number of electrons emitted, but not the KE of the electrons emitted
  • increasing frequency past the threshold increased the KE of the electrons emitted
  • the stopping voltage is equivalent to the work being done on the electrons by opposing the electric field, alongside the KE of electrons being the work done on them: K(max) = qV(stopping)
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

classical predictions of photoemission

A
  • no threshold frequency as light is dependent on intensity
  • if light did not have sufficient intensity/energy there would be a ‘time delay’ until the emission
  • if photoemission occurred, higher-intensity light would increase the number electrons emitted (photocurrent)
  • if photoemission occurred, higher intensity light would increase the max KE of electrons
  • light of any intensity and frequency would be able to release photoelectrons
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

experimental results of photoemission

A
  • there is a threshold frequency for every type of metal
  • photoelectric emission was either instantaneous or not observed
  • if photoemission occurred, higher-intensity light would increase the number of electrons emitted (photocurrent)
  • if photoemission occurred, higher frequency light would increase the max KE of electrons
  • only light of a certain frequency would be able to release photoelectrons
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

kinetic energy of electrons

A
  • by applying an electric field in the opposite direction to the electron flow in the cathode ray tube, we can adjust the electric field strength such that at a certain voltage, no electrons are able to reach the anode
  • known as stoping voltage and correlates with the maximum KE of electrons emitted
17
Q

einstein’s solution to Planck’s black body radiation

A
  • BBR is emitted in discrete packets of energy with energy, E = hf
  • proposed that all EMR was made up of packets of energy known as photons, which each carried energy E = hf
  • quantum model –> as energy was no longer dependent on intensity, however it was now proportional to frequency
18
Q

einstein’s experimental observations

A
  • suggested that photons interacted with electrons in a 1:1, all or none interaction
  • for photoemission to occur, a photon must have energy that equals or exceeds this binding energy, known as a work function of the metal
  • if photon has sufficient energy, it gives all of its energy to 1 corresponding electron, whilst extra energy is used as kinetic energy for the electron
    -if photon doesn’t have enough energy, it does not give any energy at all and emission does not occur
19
Q

einstein’s equation

A

KE = hf - W
h = 6.626 x 10^-34 Js