C13 Quantum Physics Flashcards
Max Planck’s quantum model (1900)
- EM radiation has a particulate nature, being tiny packets of energy rather than a continuous wave.
- Einstein called these packets ‘photons’.
Formula to calculate the energy of a photon
E = hf
f = frequency of the EM radiation
h = Planck’s Constant
State Planck’s Constant
6.63 x 10^-34
How to calculate energy of photon in terms of its wavelength and c
E = hc / λ
Visible Light, from longest to shortest wavelength, and energy
Red (Lowest energy)
Orange
Yellow
Green
Blue
Indigo
Violet (Highest Energy)
EM Spectrum from largest to smallest wavelength
Radio waves (Lowest Energy)
Microwaves
Infrared
Visible Light
Ultraviolet
X-ray
Gamma ray (Highest Energy)
Define the energy of 1 eV (electrovolt)
The energy transferred to or from an electron when it moves through a potential difference of 1V.
1 eV to 1J, converting between eV and J
1eV = 1.60 x 10^-19
W = VQ (Q = e)
- To convert from J to eV, divide by e
- To convert from eV to J, multiply by e
Determining Planck’s Constant
- Use a voltmeter to measure minimum p.d required to turn on LED (with black tube placed over).
- If we already know wavelength of the LED’s photons, we can determine Planck’s constant.
- eV = hc / λ
- Gather data with multiple different-wavelength LEDs (this changes threshold p.d) for accuracy.
- Plot V against 1/ λ, gradient = Planck’s constant.
Describe Photoelectric Effect
- When a photon of sufficient energy (above work function of metal) interacts with the surface of a metal, and causes a photoelectron to be emitted from its surface.
- Emission is almost instantaneous.
Gold Leaf Electroscope
- Touching top plate briefly with negative electrode charges electroscope, depositing electrons on plate and stem. Leaf stands up as it is repelled.
- UV radiation shines on a clean plate of zinc places on top, gold leaf falls back down toward stem and electroscope loses electrons and its charge.
Key observations from photoelectric effect
- Photoelectrons are only emitted if incident radiation was above threshold frequency (F0) for each metal.
- If incident radiation > F0, emission is instantaneous.
- If incident radiation > F0, increasing intensity of radiation does not affect max KE of photoelectrons, only means more will be emitted.
- The only way to increase max KE of photoelectrons is to increase frequency of incident radiation
Implications of the photoelectric affect in 1905
- The brightness of light had no effect on emission of electrons. Only frequency.
- It could not be explained by the current wave model of light, which said rate of energy transferred is dependant on brightness. Instead it was replaced by the photon model.
- Einstein proposed EM radiation as a stream of photons, not continuous waves.
Work Function
- Minimum energy required to free an electron from the surface of the metal.
How does the photon model explain the instantaneous release of photoelectrons?
- Electrons cannot accumulate energy from multiple photons, only one-to-one interactions are possible.
- As long as incident frequency > F0, photoelectrons are instantly emitted.