Study of how matter behaves at different temperatures
Clinical oxygen systems, humidification devices, ventilator circuits, etc., all rely on these principles
Hospital Liquid-Oxygen System (Real-World Example)
Large insulated outdoor silo/tank stores liquid O$_2$ at \approx -180^{\circ}C (exact value not memorised in lecture but very cold)
Piping route
Small outlet at tank base ⟶ curved pipe ⟶ underground main ⟶ bedside wall outlets
Vaporisation step
A tiny engineered hole in the pipe briefly exposes flowing liquid O$_2$ to ambient air
Even a “minuscule” temperature rise is enough to convert liquid O$_2$ to gas (dry, anhydrous)
Down-stream piping therefore carries gaseous O$_2$ only; humidification is later added at bedside
Visual clue: section of pipe exiting tank is ice-covered even on hot summer days ➜ testimony to cryogenic temperature
Vaporisation vs. Evaporation
Vaporisation = phase change liquid → gas irrespective of mechanism
Evaporation = special case of vaporisation that:
Occurs below the boiling point, at surface only
Requires heat to be taken from surrounding environment (cooling effect)
Examples
Human sweating: warm air ⟶ holds more moisture ⟶ sweat evaporates ⟶ skin cools (evaporative heat loss)
Glass of water on nightstand: water line drops over days because random surface molecules gain kinetic energy (from light/room heat) and escape into air
Boiling Point & Critical Temperature
Boiling point (BP)
Instant just before first steam bubbles / visible vapor appear
Internal vapor pressure of liquid = external barometric pressure
Critical temperature (TC)
The split-second after BP when molecules escape as visible vapor/steam
Altitude effect (Denver example)
Lower \bar P_{atm} (≈ 633\,\text{mmHg} vs. 760\,\text{mmHg} at sea level)
T_{BP} reached at lower absolute temperature ➜ foods cook longer even though water “boils sooner” (e.g.
8\,\text{min} sea-level egg ≈ 11\,\text{min} in Denver)
General rule
P{vapor}=P{atm}\;\Rightarrow\;\text{boiling begins}
Temperature Scales & Conversions
Kelvin (K)
Absolute scale, 0\,\text K = -273^{\circ}C (absolute zero)
Used in research/teaching hospitals (UCLA, UCI etc.)
Clinical practice alternates between °F & °C
Key conversions
^{\circ}C = (^{\circ}F - 32)/1.8
^{\circ}F = (^{\circ}C \times 1.8) + 32
Examples
Normal body temp 98.6^{\circ}F \Rightarrow 37^{\circ}C
Drop of 1^{\circ}C represents larger thermal change than drop of 1^{\circ}F
Condensation & Humidity Basics
Condensation = gas cools ⟶ water droplets form (reverse of evaporation)
Seen on windshields, iced drink glasses, ventilator circuits when heater too low
To minimise circuit rainout ➜ increase humidifier temperature closer to 37^{\circ}C
Pascal, Buoyancy & Archimedes (Liquids)
Pascal’s Principle
P = \rho g h ; pressure exerted by a liquid depends on density and depth
Archimedes / Buoyancy
Upward buoyant force B = \rho{water} \times V{displaced}
Object appears lighter in water; force under object > atmospheric force above
Bernoulli’s Principle (applies to liquids and gases)
In a narrowing tube: pressure lateral to flow decreases, velocity & momentum increase ➜ transition from turbulent (large lumen) to laminar (small lumen)