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Experimental Physics2026-07-13

Vacuum Technology

Vacuum Generation

Vacuum systems are categorized by pressure range:

RegimePressure RangeTypical Pump
Rough Vacuum10310^31Pa1 \, \text{Pa}Rotary vane
Medium Vacuum11103Pa10^{-3} \, \text{Pa}Turbomolecular
High Vacuum10310^{-3}107Pa10^{-7} \, \text{Pa}Diffusion / Turbo
Ultra-High Vacuum<107Pa< 10^{-7} \, \text{Pa}Ion pump + Ti sublimation

Pressure Measurement

The mean free path of gas molecules relates to pressure:

λ=kBT2πd2P\lambda = \frac{k_B T}{\sqrt{2} \pi d^2 P}

where dd is the molecular diameter and PP is pressure.

Cryogenics

Gas Liquefaction

The Joule-Thomson coefficient determines whether a gas cools or heats upon expansion:

μJT=(TP)H\mu_{JT} = \left(\frac{\partial T}{\partial P}\right)_H

For gases below their inversion temperature, μJT>0\mu_{JT} > 0 and expansion causes cooling.

Superfluidity

Liquid helium-4 undergoes a phase transition at the lambda point (Tλ=2.17KT_\lambda = 2.17 \, \text{K}), entering a superfluid state with zero viscosity.

Thermometry

Resistance Thermometers

The resistance of platinum follows the Callendar-Van Dusen equation:

R(T)=R0[1+AT+BT2+C(T100)T3]R(T) = R_0 \left[1 + A T + B T^2 + C(T-100)T^3\right]

for T<0°CT < 0°\text{C}, where R0=100ΩR_0 = 100 \, \Omega for a Pt100 sensor.

Optics & Spectroscopy

Laser Fundamentals

Population inversion is the key condition for lasing:

N2>N1N_2 > N_1

where N2N_2 and N1N_1 are populations of the upper and lower laser states.

Atomic Spectra

The energy levels of hydrogen-like atoms:

En=13.6eVn2Z2E_n = -\frac{13.6 \, \text{eV}}{n^2} \cdot Z^2

Particle & Photon Detection

Photomultiplier Tubes

PMTs achieve single-photon detection through cascading secondary electron emission. The gain is:

G=δnG = \delta^n

where δ\delta is the secondary emission coefficient per dynode and nn is the number of dynode stages (typically 8–14).

Source

Notes structured as an Obsidian vault with cross-linked concepts. Available on GitHub.