Atmospheric Moisture, Humidity & Dew Point — Summary Notes
1. Water Vapour in the Atmosphere
Water vapour (H₂O) is the most important atmospheric gas from a weather and meteorological standpoint.
- It is highly variable, ranging from almost 0% to about 4–5% by volume.
- It is the only atmospheric substance that naturally occurs in all three states:
- Solid: Ice
- Liquid: Water
- Gas: Water vapour
- Water vapour is essential for:
- Cloud formation
- Fog and mist formation
- Dew formation
- Precipitation
- Atmospheric energy transfer
- Changes of state involve latent heat, which is an important source of atmospheric energy.
- Latent heat release is particularly important in:
- Convection
- Thunderstorms
- Hurricanes
- Cloud development
- The difference between the Dry Adiabatic Lapse Rate (DALR) and Moist/Saturated Adiabatic Lapse Rate (MALR/SALR).
Key Point
Water vapour → moisture, clouds, precipitation and latent-heat energy.
2. Relative Humidity (RH)
Relative Humidity is the ratio of the actual water vapour content of air to the maximum amount of water vapour the air can hold at its current temperature and pressure, expressed as a percentage.
Formula
RH = (Actual Water Vapour Content / Maximum Water Vapour Capacity) × 100%
RH can also be expressed as:
RH = (HMR / SMR) × 100%
or:
RH = (Actual Vapour Pressure / Saturation Vapour Pressure) × 100%
Where:
- HMR = Humidity Mixing Ratio
- SMR = Saturation Mixing Ratio
What RH Tells Us
RH indicates how close the air is to saturation.
It does not directly indicate the total amount of water vapour present.
Saturation
- RH = 100% → air is saturated.
- RH < 100% → air is unsaturated/dry.
- Even 99% RH is technically classified as unsaturated or dry air.
3. Factors Affecting Relative Humidity
RH can change in two principal ways:
- By changing the actual water vapour content
- By changing the air temperature
If Temperature Remains Constant
Adding water vapour:
Moisture ↑ → RH ↑
Removing water vapour:
Moisture ↓ → RH ↓
If Moisture Content Remains Constant
Warming the air:
Temperature ↑ → Capacity ↑ → RH ↓
Cooling the air:
Temperature ↓ → Capacity ↓ → RH ↑
Important Relationship
With constant moisture content, RH is inversely related to temperature.
4. Saturation Capacity of Air
The maximum amount of water vapour that air can contain is called its saturation capacity.
It is primarily controlled by temperature.
Relationship
Temperature ↑ → Saturation capacity ↑
Temperature ↓ → Saturation capacity ↓
Warmer air can hold more water vapour before reaching saturation.
Saturation capacity can be represented by:
- Saturation Content
- Saturation Vapour Pressure
5. Absolute Humidity
Absolute Humidity (AH) is the actual mass of water vapour contained in a unit volume of air.
Formula Concept
AH = Mass of water vapour / Volume of air
Unit
Usually:
g/m³
Important Distinction
| Term | Meaning | Typical Unit |
|---|---|---|
| Absolute Humidity | Actual mass of water vapour per unit volume | g/m³ |
| Relative Humidity | Degree of saturation | % |
| Humidity Mixing Ratio | Mass of water vapour per mass of dry air | g/kg |
| Specific Humidity | Mass of water vapour per mass of total air | g/kg |
AH represents the physical concentration of water vapour, whereas RH represents how close the air is to saturation.
6. Humidity Mixing Ratio (HMR)
Humidity Mixing Ratio is the mass of water vapour contained in a unit mass of dry air.
Formula
HMR = Mass of water vapour / Mass of dry air
Unit
Usually:
g/kg
During Unsaturated Adiabatic Ascent
When unsaturated air rises:
- Pressure decreases.
- Air expands.
- Temperature decreases.
- No moisture is exchanged with the surroundings.
- Mass of water vapour remains constant.
- Mass of dry air remains constant.
- Therefore, HMR remains constant.
7. Specific Humidity
Specific humidity represents the mass of water vapour relative to the total mass of air.
During an unsaturated adiabatic ascent, there is no exchange of mass with the surroundings, so:
Specific Humidity remains constant.
Compare
- HMR: water vapour / dry air
- Specific Humidity: water vapour / total air
8. Dew Point Temperature
Dew Point (DP) is the temperature to which air must be cooled, at constant pressure and constant water vapour content, to become saturated.
At the dew point:
RH = 100%
and:
Air Temperature = Dew Point
Relationship
T ≥ DP
Therefore:
- Saturated air → T = DP
- Unsaturated air → T > DP
- Dew point can never exceed air temperature.
Importance of Dew Point
Dew point is a direct indicator of the actual moisture content of the air.
Higher DP → greater actual moisture content.
9. Temperature–Dew Point Spread
The difference between air temperature and dew point is called the temperature–dew point spread.
Formula
Spread = T − DP
| Spread | RH / Moisture Condition |
|---|---|
| Large spread | Low RH; air is far from saturation |
| Small spread | High RH; air is close to saturation |
| Zero spread | RH = 100%; saturated |
Most Important Rule
T = DP → RH = 100% → Saturation
A decreasing spread indicates that the air is approaching saturation and therefore increases the possibility of:
- Fog
- Mist
- Dew
- Cloud formation
10. Example: Calculating Cooling Required for Saturation
Given:
- Air temperature = +12°C
- Dew point = +5°C
Required cooling:
12 − 5 = 7°C
Therefore, the air must cool by 7°C to reach saturation.
At +5°C:
- T = DP
- RH = 100%
- Air is saturated.
Further cooling can result in condensation.
11. Dew Point and Moisture Content
Dew point is primarily controlled by the actual water vapour content.
If air is simply heated or cooled without adding or removing moisture:
- Actual moisture content remains unchanged.
- Dew point remains constant.
- RH changes because the saturation capacity changes with temperature.
Example: Clear Night
During a clear night:
- Temperature decreases.
- Air capacity to hold water vapour decreases.
- RH increases.
- Dew point does not change, provided no moisture is added or removed.
12. Dew Point During Ascent
The source gives a theoretical dew-point lapse rate of approximately:
0.5°C per 1,000 ft
Therefore, as air rises, the dew point generally decreases at approximately:
0.5°C / 1,000 ft
This is distinct from the temperature lapse rate of the air parcel.
13. Unsaturated Air Rising Adiabatically
When an unsaturated air parcel rises:
- Atmospheric pressure decreases.
- The parcel expands.
- The parcel cools at the Dry Adiabatic Lapse Rate (DALR).
- No moisture is exchanged with the surroundings.
- HMR remains constant.
- Specific humidity remains constant.
- Air’s moisture-holding capacity decreases.
- RH increases.
- The parcel eventually reaches RH = 100% at the condensation level.
Absolute Humidity
As the parcel rises:
- Volume increases because of expansion.
- Water vapour mass remains constant.
- Therefore, absolute humidity decreases.
14. Descending Air
When air descends:
- Ambient pressure increases.
- Air is compressed.
- Compression causes adiabatic warming.
- Actual moisture content remains constant, assuming no moisture is added or removed.
- Warmer air has a greater moisture-holding capacity.
- RH therefore decreases.
- The air moves farther away from saturation.
Memory Rule
Descending air → warming → capacity increases → RH decreases.
15. Saturated vs Unsaturated Air
| Condition | Relative Humidity | Temperature / DP |
|---|---|---|
| Saturated air | 100% | T = DP |
| Unsaturated air | <100% | T > DP |
Important Examination Point
Air with 95% or 99% RH is still unsaturated/dry air because it has not reached 100% saturation.
Unsaturated air cools at the:
Dry Adiabatic Lapse Rate (DALR)
16. Condensation
Condensation is the change of state:
Water vapour → Liquid water
It is an exothermic process, meaning it releases latent heat.
Effects
The released latent heat:
- Warms the surrounding air.
- Adds energy to the atmosphere.
- Slows the cooling of rising saturated air.
- Reduces the lapse rate compared with dry adiabatic cooling.
- Supports buoyancy and cloud development.
Aviation Significance
Condensation contributes to the formation of:
- Clouds
- Fog
- Mist
- Dew
17. Latent Heat and Saturated Adiabatic Lapse Rate
During condensation:
Latent heat is released.
This heat partially offsets the cooling of rising saturated air.
Therefore:
SALR/MALR < DALR
In other words:
Saturated air cools more slowly with height than dry air.
The amount of latent heat released depends on the amount of water vapour that condenses.
More condensation → more latent heat released.
18. Evaporation
Evaporation is the change of state:
Liquid water → Water vapour
Evaporation requires energy.
Therefore:
Latent heat is absorbed.
The energy is taken from the surrounding environment, producing a cooling effect.
Memory Rule
Evaporation → absorbs heat → cooling
Condensation → releases heat → warming
19. Sublimation and Deposition
Sublimation
Direct change:
Ice → Water vapour
- Liquid state is bypassed.
- Latent heat is absorbed.
Deposition
Direct change:
Water vapour → Ice
- Liquid state is bypassed.
- Latent heat is released.
The source also refers to the gas-to-solid process as sublimation or deposition.
Aviation Relevance
Deposition contributes to hoarfrost/frost formation when temperature and dew/frost point are below freezing.
20. Saturation Vapour Pressure Over Water and Ice
At the same temperature below 0°C:
SVP over liquid water > SVP over ice
Reason
Water molecules escape more easily from a liquid water surface than from an ice surface.
Therefore, a greater vapour pressure is required to saturate air over liquid water than over ice at the same sub-freezing temperature.
Importance
This difference forms the basis of the Ice-Crystal / Bergeron Process, where ice crystals can grow at the expense of surrounding supercooled water droplets and contribute to precipitation formation in cold clouds.
21. Diurnal Variation of Relative Humidity
The daily variation of RH is mainly controlled by the daily temperature cycle, assuming actual moisture content remains approximately constant.
Daytime
Solar heating causes:
Temperature ↑ → Moisture-holding capacity ↑ → RH ↓
- RH decreases as temperature rises.
- Lowest RH generally occurs around 1500 LMT, when temperature is near its daily maximum.
Nighttime / Early Morning
Cooling causes:
Temperature ↓ → Capacity ↓ → RH ↑
- RH increases during the night.
- Highest RH occurs around the coolest part of the day.
- The source specifies approximately 30 minutes after sunrise, when temperature is minimum.
Operational Significance
High RH during the night and early morning increases the possibility of:
- Fog
- Mist
- Dew
- Other condensation phenomena
22. Relative Humidity and Temperature — Quick Table
| Situation | Temperature | Capacity | RH |
|---|---|---|---|
| Air warmed, moisture constant | ↑ | ↑ | ↓ |
| Air cooled, moisture constant | ↓ | ↓ | ↑ |
| Moisture added, temperature constant | — | — | ↑ |
| Moisture removed, temperature constant | — | — | ↓ |
| T approaches DP | ↓ | ↓ | ↑ toward 100% |
| T = DP | — | — | 100% |
23. Wet-Bulb Temperature
Wet-Bulb Temperature (Tᵂ) is the lowest temperature to which air can be cooled by evaporation of water.
It is measured using a wet-bulb thermometer, which forms part of a:
Psychrometer / Wet-and-Dry-Bulb Hygrometer
How It Works
- The thermometer bulb is covered by a wet muslin wick.
- Water evaporates from the wick when the air is unsaturated.
- Evaporation absorbs latent heat.
- Heat is removed from the thermometer bulb.
- The wet-bulb temperature falls below the dry-bulb temperature.
24. Wet-Bulb Depression
Wet-Bulb Depression is the difference between:
Dry-Bulb Temperature − Wet-Bulb Temperature
In Unsaturated Air
- Evaporation occurs.
- Latent heat is absorbed.
- Wet-bulb temperature is lower than dry-bulb temperature.
In Saturated Air
When:
RH = 100%
- No net evaporation occurs.
- No additional latent heat is absorbed.
- Wet-bulb temperature equals dry-bulb temperature.
At saturation:
Dry Bulb Temperature = Wet Bulb Temperature = Dew Point
25. Wet Bulb vs Dew Point
The two temperatures should not be confused.
| Parameter | Wet-Bulb Temperature | Dew Point |
|---|---|---|
| Definition | Lowest temperature attainable by evaporation | Temperature required to reach saturation by cooling |
| Main process | Evaporation | Cooling |
| Measurement | Wet-bulb thermometer | Psychrometer-derived |
| Normally | Between dry bulb and dew point | ≤ air temperature |
| At saturation | WBT = DBT = DP | DP = DBT |
Important
Wet-bulb temperature is generally not equal to dew point.
They become equal only at saturation.
26. Psychrometer / Hygrometer
A hygrometer is an instrument used to measure atmospheric moisture/humidity.
Examples include:
- Hair hygrometer
- Electrical hygrometer
- Psychrometer
A psychrometer consists of:
- Dry-bulb thermometer
- Wet-bulb thermometer
The difference between the dry- and wet-bulb temperatures, known as wet-bulb depression, is used to determine:
- Relative Humidity
- Dew Point
- Humidity Mixing Ratio
Saturation Check
If:
RH = 100%
then:
Dry Bulb = Wet Bulb = Dew Point
27. Why Does the Wet Bulb Cool?
In unsaturated air:
- Water evaporates from the wet muslin wick.
- Evaporation requires latent heat.
- Latent heat is absorbed from the surrounding environment and thermometer bulb.
- The bulb loses sensible heat.
- Its temperature falls.
- The lowest temperature reached is the wet-bulb temperature.
Key Rule
Greater evaporation → greater wet-bulb depression.
At saturation, evaporation stops and:
Wet-bulb depression = 0
28. Troposphere and Atmospheric Moisture
The troposphere contains virtually all of the atmosphere’s water vapour.
Troposphere
- Extends from the surface to the tropopause.
- Average tropopause height is approximately 11 km.
- Contains almost all atmospheric moisture.
- Temperature generally decreases with altitude.
- Almost all normal weather occurs in this layer.
Stratosphere
- Located above the tropopause.
- Contains very little moisture.
- Generally lacks clouds, apart from rare cloud types such as nacreous clouds.
Tropopause
The boundary between:
Troposphere ↔ Stratosphere
It is associated with an abrupt change in the temperature lapse-rate characteristics.
29. Rain and Runway Performance
On a rainy day, required runway length can increase for both takeoff and landing.
Two main factors are involved.
Takeoff
Rain is often associated with high humidity.
Higher moisture content can contribute to lower air density because water vapour is less dense than dry air.
Lower density results in:
- Reduced aerodynamic lift
- Reduced engine performance/thrust
- Higher density altitude
- Longer takeoff distance
Landing
Rain produces a wet runway.
A wet runway can cause:
- Reduced tyre/runway friction
- Reduced braking effectiveness
- Aquaplaning/hydroplaning risk
- Increased landing roll
Overall Result
Low-density air + wet runway → greater required runway length.
30. High-Value Relationships
Relative Humidity
RH ↑ when temperature ↓, if moisture content is constant.
Moisture Addition
Moisture ↑ → RH ↑, if temperature is constant.
Moisture Removal
Moisture ↓ → RH ↓, if temperature is constant.
Saturation
T = DP → RH = 100%
Unsaturated Air
T > DP → RH < 100%
Dew Point
Higher DP → Higher actual moisture content
Temperature–Dew Point Spread
Large spread → Low RH
Small spread → High RH
Zero spread → RH 100%
Rising Unsaturated Air
Rising → cooling → RH ↑
Descending Air
Descending → warming → RH ↓
Phase Changes
Evaporation → latent heat absorbed → cooling
Condensation → latent heat released → warming
Ice → vapour → latent heat absorbed
Vapour → ice → latent heat released
31. Important Numerical Values
| Parameter | Value |
|---|---|
| Maximum atmospheric water vapour content | About 4–5% by volume |
| Average tropopause height | About 11 km |
| Dew-point lapse rate | About 0.5°C / 1,000 ft |
| Typical lowest RH | Around 1500 LMT |
| Typical highest RH | Around 30 min after sunrise |
| Saturation RH | 100% |
32. Exam Quick Revision Table
| Question Concept | Correct Relationship |
|---|---|
| What is RH? | Actual moisture / maximum capacity × 100 |
| RH = 100% | Saturated air |
| RH = 99% | Still unsaturated/dry air |
| What controls saturation capacity? | Mainly temperature |
| Temperature increases | Moisture capacity increases |
| Temperature decreases | Moisture capacity decreases |
| Moisture constant + temperature increases | RH decreases |
| Moisture constant + temperature decreases | RH increases |
| Moisture added at constant temperature | RH increases |
| Moisture removed at constant temperature | RH decreases |
| What does DP indicate? | Actual moisture content |
| High DP | High moisture content |
| T = DP | Saturation / RH 100% |
| T > DP | Unsaturated air |
| DP > T | Not possible |
| Large T–DP spread | Low RH |
| Small T–DP spread | High RH |
| Zero T–DP spread | RH 100% |
| Unsaturated air rising | Cools at DALR |
| HMR during unsaturated ascent | Constant |
| Specific humidity during unsaturated ascent | Constant |
| RH during unsaturated ascent | Increases |
| Absolute humidity during ascent | Decreases due to expansion |
| Descending air | Compresses and warms |
| RH during descent | Decreases |
| Condensation | Vapour → liquid |
| Condensation heat | Released |
| Evaporation | Liquid → vapour |
| Evaporation heat | Absorbed |
| Deposition | Vapour → ice |
| Deposition heat | Released |
| Sublimation | Ice → vapour |
| SVP below 0°C | Water > Ice |
| Main humidity instrument | Hygrometer |
| Wet + dry bulb instrument | Psychrometer |
| RH 100% | DBT = WBT = DP |
| Wet-bulb depression | DBT − WBT |
| Rainy-day takeoff | Longer distance due partly to lower density/performance |
| Rainy-day landing | Longer roll due to wet runway/reduced braking |
33. One-Minute Memory Sheet
RH = Actual moisture / Capacity × 100
RH 100% = Saturated
T = DP = 100% RH
DP can never be higher than T
High DP = High moisture
Large T–DP spread = Low RH
Small T–DP spread = High RH
Cooling → RH increases
Warming → RH decreases
(when moisture content is constant)
Adding moisture → RH increases
Rising unsaturated air → cools → RH increases
Descending air → warms → RH decreases
HMR remains constant during unsaturated adiabatic ascent
Condensation → releases latent heat
Evaporation → absorbs latent heat
Saturated air cools more slowly than dry air
DBT = WBT = DP at saturation
Water vapour → liquid = condensation
Liquid water → vapour = evaporation
Vapour → ice = deposition
Ice → vapour = sublimation
Below 0°C: SVP over water > SVP over ice
Troposphere contains virtually all atmospheric water vapour