physics / light-matter-ref.mdon commit light-matter cheatsheet (ba45d5d)
   1---
   2geometry: margin=2cm
   3columns: 2
   4graphics: yes
   5author: Andrew Lorimer
   6---
   7
   8\pagenumbering{gobble}
   9\usepackage{multicols}
  10
  11# Light and Matter
  12
  13## Planck's equation
  14
  15$$f={c \over \lambda}$$
  16
  17$$E=hf={hc \over \lambda}$$
  18
  19$$h=6.63 \times 10^{-34}\operatorname{J s}=4.12 \times 10^{-15} \operatorname{eV s}$$
  20
  21## Force of electrons
  22
  23$$F=evB$$
  24
  25## Photoelectric effect
  26
  27- $V_{\operatorname{supply}}$ does not affect photocurrent
  28- if $V_{\operatorname{supply}} > 0$, e- are attracted to collector anode
  29- if $V_{\operatorname{supply}} < 0$, e- are attracted to illuminated cathode, and $I\rightarrow 0$
  30- $v$ of e- depends on ionisation energy (shell)
  31
  32### Threshold frequency
  33- *threshold frequency* $f_0$ - minimum frequency for photoelectrons to be ejected
  34- $x$-intercept of frequency vs $E_K$ graph
  35- if $f < f_0$, no photoelectrons are detected
  36
  37### Work function
  38- *work function* $\phi$ - minimum energy required to release photoelectrons
  39- magnitude of $y$-intercept of frequency vs $E_K$ graph
  40- $\phi$ is determined by strength of bonding
  41
  42$$\phi=hf_0$$
  43
  44### Kinetic energy
  45
  46$$E_{\operatorname{k-max}}=hf - \phi$$
  47
  48voltage in circuit = max $E_K$ in eV
  49
  50### Stopping potential
  51
  52_Smallest voltage to achieve minimum current_
  53
  54$$V_0 = {E_{K \operatorname{max}} \over q_e} = {{hf - \phi} \over q_e}$$
  55
  56## De Broglie's theory
  57
  58$$\lambda = {h \over \rho} = {h \over mv}$$
  59$$\rho = {hf \over c} = {h \over \lambda}$$
  60$$E = \rho c$$
  61
  62- impossible to confirm de Broglie's theory of matter with double-slit experiment, since wavelengths are much smaller than for light, requiring an equally small slit ($< r_{\operatorname{proton}}$)
  63- confirmed by Davisson and Germer's apparatus (diffraction pattern like double-slit)
  64- also confirmed by Thomson - e- diffraction pattern resembles x-ray (wave) pattern
  65
  66## X-ray and electron interaction
  67
  68- electron is only stable in orbit if $mvr = n{h \over 2\pi}$ where $n \in \mathbb{Z}$
  69- rearranging this, $2\pi r = n{h \over mv}$ (circumference)
  70- if $2\pi r \ne n{h \over mv}$, interference occurs, standing wave cannot be established
  71
  72## Spectral analysis
  73
  74<!-- ![](graphics/energy-levels.png) -->
  75- $\Delta E = hf = {hc \over \lambda}$ between ground / excited state
  76- $f$ of a photon emitted or absorbed can be calculated from energy difference: $E_2 – E_1 = hf$ or $= hc$
  77- Ionisation energy - min $E$ required to remove e-
  78- EMR is absorbed/emitted when $E_{\operatorname{K-in}}=\Delta E_{\operatorname{shells}}$ (i.e. $\lambda = {hc \over \Delta E_{\operatorname{shells}}}$)
  79
  80## Indeterminancy principle
  81
  82measuring location of an e- requires hitting it with a photon, but this causes $\rho$ to be transferred to electron, moving it. $\therefore, \sigma E \propto {1 \over \sigma t}$
  83
  84$$\sigma E \sigma t \ge {h \over 4 \pi}$$
  85
  86## Wave-particle duality
  87wave model:  
  88
  89- cannot explain photoelectric effect
  90- $f$ is irrelevant to photocurrent
  91- predicts delay between incidence and ejection
  92- speed depends on medium
  93
  94particle model:  
  95
  96- explains photoelectric effect
  97- rate of photoelectron release $\propto$ intensity
  98- no time delay - one photon releases one electron
  99- double slit: photons interact as they pass through slits. interference pattern still appears when a dim light source is used so that only one photon can pass at a time
 100- light exerts force
 101- light bent by gravity