HVAC Systems Encyclopedia

A comprehensive encyclopedia of heating, ventilation, and air conditioning systems

Fluid Properties

Fluid properties define the physical and thermodynamic characteristics that govern fluid behavior in HVAC systems. These properties determine flow rates, pressure drops, heat transfer effectiveness, pump and fan performance, and system energy consumption. Accurate knowledge of fluid properties at operating conditions is critical for proper system design, equipment selection, and performance prediction.

Density

Density (ρ) represents the mass per unit volume of a fluid and directly affects momentum, pressure drop, and buoyancy forces in HVAC systems.

Definition:

ρ = m/V

Where:

  • ρ = density (lbm/ft³ or kg/m³)
  • m = mass (lbm or kg)
  • V = volume (ft³ or m³)

Temperature Effects on Density

All fluids exhibit density variations with temperature. For liquids, density decreases with increasing temperature. For gases, density is inversely proportional to absolute temperature per the ideal gas law.

Ideal Gas Law:

ρ = P/(R·T)

Where:

  • P = absolute pressure (psia or Pa)
  • R = specific gas constant (ft·lbf/(lbm·°R) or J/(kg·K))
  • T = absolute temperature (°R or K)

Density Values for Common HVAC Fluids

FluidTemperature (°F)Density (lbm/ft³)Notes
Water3262.42Maximum density at 39.2°F
Water6062.37Standard reference
Water10062.00Cooling water systems
Water18060.57Hot water heating
Water20060.12High temperature systems
Air (sea level)700.0749Standard conditions
Air (sea level)00.0862Cold outdoor air
R-134a liquid4079.89Saturated liquid
R-410A liquid4070.76Saturated liquid
30% Ethylene Glycol4064.89Freeze protection to 15°F
50% Propylene Glycol4065.26Freeze protection to -28°F

ASHRAE Reference: ASHRAE Handbook - Fundamentals, Chapter 33 (Thermophysical Properties of Refrigerants) and Chapter 34 (Psychrometrics)

Altitude Effects on Air Density

Air density decreases with elevation, affecting fan performance and air-side heat transfer:

ρ_altitude = ρ_std · (1 - 6.87 × 10^-6 · h)^5.26

Where h = elevation above sea level (ft)

Specific Gravity

Specific gravity (SG) is the dimensionless ratio of fluid density to the density of water at standard conditions (60°F, 62.37 lbm/ft³).

SG = ρ_fluid / ρ_water

Specific gravity is particularly important for:

  • Glycol solution concentrations
  • Refrigerant charge calculations
  • Pump NPSH requirements
  • Hydronic system design

Specific Gravity Values

FluidTemperature (°F)Specific GravityApplication
Water601.000Reference standard
Ethylene Glycol (100%)601.115Antifreeze concentrate
Propylene Glycol (100%)601.036Antifreeze concentrate
30% Ethylene Glycol601.040Typical freeze protection
R-134a liquid401.28Refrigerant systems
Mercury6013.55Pressure measurement

Specific Weight

Specific weight (γ) represents the weight per unit volume:

γ = ρ·g

Where:

  • γ = specific weight (lbf/ft³ or N/m³)
  • g = gravitational acceleration (32.174 ft/s² or 9.807 m/s²)

Specific weight is used in hydrostatic pressure calculations and pump head determinations. For water at 60°F: γ = 62.37 lbf/ft³.

Viscosity

Viscosity quantifies a fluid’s resistance to flow and internal shearing forces. It directly impacts pressure drop, pumping power, heat transfer coefficients, and flow regime determination.

Dynamic (Absolute) Viscosity

Dynamic viscosity (μ) represents the ratio of shear stress to shear rate in a fluid:

τ = μ · (du/dy)

Where:

  • τ = shear stress (lbf/ft² or Pa)
  • μ = dynamic viscosity (lbm/(ft·s), cP, or Pa·s)
  • du/dy = velocity gradient perpendicular to flow (s^-1)

Unit Conversions:

  • 1 centipoise (cP) = 0.000672 lbm/(ft·s)
  • 1 Pa·s = 1000 cP
  • 1 lbm/(ft·s) = 1488.2 cP

Kinematic Viscosity

Kinematic viscosity (ν) is the ratio of dynamic viscosity to density:

ν = μ/ρ

Where:

  • ν = kinematic viscosity (ft²/s, cSt, or m²/s)
  • 1 centistoke (cSt) = 1.076 × 10^-5 ft²/s

Kinematic viscosity is used in Reynolds number calculations and appears in the Navier-Stokes equations.

Viscosity Values for HVAC Fluids

FluidTemp (°F)Dynamic Viscosity (cP)Kinematic Viscosity (cSt)
Water321.791.93
Water601.121.22
Water1000.680.74
Water1800.350.39
Air320.017113.23
Air700.018116.15
Air2120.022033.44
30% Ethylene Glycol403.243.37
50% Propylene Glycol406.106.31
R-134a liquid400.2700.228

Temperature Effects on Viscosity

Liquids: Viscosity decreases exponentially with temperature:

μ = A · e^(B/T)

Where A and B are empirical constants specific to each fluid.

Gases: Viscosity increases with temperature per Sutherland’s law:

μ = μ_0 · (T/T_0)^(3/2) · [(T_0 + S)/(T + S)]

For air: S = 110.4 K (Sutherland constant)

ASHRAE Reference: ASHRAE Handbook - Fundamentals, Chapter 1 (Psychrometrics), provides detailed viscosity correlations.

Newtonian vs. Non-Newtonian Fluids

Newtonian Fluids

Newtonian fluids exhibit constant viscosity regardless of shear rate. The shear stress is directly proportional to shear rate. Most HVAC fluids are Newtonian:

  • Water
  • Air
  • Refrigerants
  • Glycol solutions (at typical concentrations)
  • Hydronic oils

Standard pipe friction correlations (Darcy-Weisbach, Colebrook equation) apply directly to Newtonian fluids.

Non-Newtonian Fluids

Non-Newtonian fluids exhibit viscosity changes with shear rate. Examples in specialized HVAC applications:

  • High-concentration polymeric additives
  • Some thermal storage phase-change materials
  • Certain heat transfer fluids at extreme temperatures

Types:

  1. Pseudoplastic (shear-thinning): viscosity decreases with shear rate
  2. Dilatant (shear-thickening): viscosity increases with shear rate
  3. Bingham plastic: requires threshold stress before flow begins

Non-Newtonian behavior requires specialized friction factor correlations and computational fluid dynamics analysis.

Compressibility

Compressibility quantifies the volume change of a fluid under pressure variations.

Bulk Modulus of Elasticity

The bulk modulus (K or β) measures resistance to compression:

K = -V · (dP/dV) = ρ · (dP/dρ)

Where:

  • K = bulk modulus (psi or Pa)
  • V = volume
  • P = pressure

Practical Values:

FluidTemperature (°F)Bulk Modulus (psi)Compressibility
Water60320,000Nearly incompressible
Water200270,000Decreases with temperature
Ethylene Glycol60420,000Less compressible than water
Air6014.7 (at 1 atm)Highly compressible
Hydraulic Oil60250,000Used in controls

Compressibility Coefficient

β = 1/K = -(1/V) · (dV/dP)

For liquids in hydronic systems, compressibility is typically negligible in pressure drop calculations but becomes important in:

  • Water hammer analysis
  • Expansion tank sizing
  • Pressure surge protection
  • Acoustic wave propagation

ASHRAE Reference: ASHRAE Handbook - HVAC Systems and Equipment, Chapter 13 (Hydronic Heating and Cooling Systems)

Speed of Sound

The speed of sound in a fluid relates directly to compressibility:

c = √(K/ρ)

For water at 60°F: c ≈ 4,900 ft/s For air at 70°F: c ≈ 1,130 ft/s

Coefficient of Thermal Expansion

The volumetric coefficient of thermal expansion (β_T) quantifies volume change with temperature:

β_T = (1/V) · (dV/dT)_P

Or for density:

β_T = -(1/ρ) · (dρ/dT)_P

Thermal Expansion Values

FluidTemperature Range (°F)β_T (1/°F)Application Impact
Water40-2002.1 × 10^-4Expansion tank sizing
Ethylene Glycol40-2003.5 × 10^-4Larger expansion tanks
Propylene Glycol40-2003.8 × 10^-4Larger expansion tanks
Air (ideal gas)All1/T_absDensity altitude correction

Hydronic System Expansion Volume

The total expansion volume in a closed hydronic system:

V_exp = V_sys · β_T · ΔT

Where:

  • V_exp = expansion volume (gal)
  • V_sys = total system volume (gal)
  • ΔT = temperature change from fill to maximum operating (°F)

This calculation is critical for expansion tank selection per ASHRAE Standard 12 (Minimizing the Risk of Legionellosis).

Surface Tension

Surface tension (σ) is the force per unit length at the interface between liquid and gas:

σ = F/L

Units: lbf/ft, dyne/cm, or N/m

Surface Tension Values

FluidTemperature (°F)Surface Tension (dyne/cm)
Water6073.0
Water21258.9
Ethylene Glycol6048.4
R-134a4012.3

HVAC Applications:

  • Droplet formation in cooling coils
  • Condensate drainage behavior
  • Evaporative cooling effectiveness
  • Spray nozzle atomization
  • Drain pan design

Capillarity

Capillary action results from the combination of surface tension and adhesive forces between liquid and solid surfaces.

Capillary Rise

The height of capillary rise in a tube:

h = (2·σ·cos θ)/(ρ·g·r)

Where:

  • h = capillary rise height (ft)
  • σ = surface tension (lbf/ft)
  • θ = contact angle (degrees)
  • r = tube radius (ft)

HVAC Relevance:

  • Condensate drainage in small tubes
  • Wicking in insulation materials
  • Drain line trap seal maintenance
  • Microgroove heat exchanger design

Vapor Pressure

Vapor pressure is the pressure exerted by a vapor in equilibrium with its liquid phase at a given temperature. It increases exponentially with temperature.

Antoine Equation

log₁₀(P_vap) = A - B/(C + T)

Where A, B, C are substance-specific constants.

Vapor Pressure Values for Water

Temperature (°F)Vapor Pressure (psia)Significance
320.0887Freezing point
600.2563Standard conditions
1000.9503Cooling tower range
1807.510Hot water systems
21214.696Atmospheric boiling

ASHRAE Reference: ASHRAE Handbook - Fundamentals, Chapter 1 (Psychrometrics), Steam tables

HVAC Design Implications

  1. NPSH Requirements: Net Positive Suction Head must exceed vapor pressure to prevent cavitation:

    NPSH_available = P_atm + P_static - P_friction - P_vapor

  2. Cooling Tower Performance: Wet bulb temperature approach limited by vapor pressure differential

  3. Dehumidification: Coil surface temperature must be below dewpoint (vapor pressure determines saturation)

  4. Vacuum Systems: Steam condensers operate below atmospheric pressure

Cavitation Phenomenon

Cavitation occurs when local pressure in a liquid drops below vapor pressure, causing vapor bubble formation, subsequent collapse, and potential equipment damage.

Cavitation Index

The Thoma cavitation parameter (σ):

σ = (NPSH_available)/(H_pump)

Where H_pump = total pump head developed (ft)

Cavitation risk increases when σ < σ_critical (typically 0.1-0.4 for centrifugal pumps)

Cavitation Prevention Strategies

  1. Increase NPSH_available:

    • Elevate fluid source above pump
    • Minimize suction line friction
    • Reduce suction line length
    • Increase pipe diameter
    • Lower fluid temperature
  2. System Design:

    • Position pumps at lowest point
    • Use suction diffusers
    • Avoid elbows near pump inlet
    • Provide adequate submergence in open systems
  3. Pump Selection:

    • Select pumps with low NPSH_required
    • Use double-suction impellers
    • Consider inducer-equipped pumps

ASHRAE Reference: ASHRAE Handbook - HVAC Systems and Equipment, Chapter 44 (Pumps)

Cavitation Damage Indicators

  • High-frequency noise and vibration (sounds like gravel)
  • Reduced pump performance
  • Eroded impeller surfaces (pitting)
  • Mechanical seal failure
  • Bearing damage

Pressure-Temperature-Density Relationships

Incompressible Flow Assumption

For liquids in hydronic systems, density remains constant:

ρ ≈ constant (for ΔP « 1000 psi)

This assumption simplifies:

  • Bernoulli equation application
  • Pump head calculations
  • Pipe sizing procedures
  • Flow measurement

Compressible Flow Criteria

Air and refrigerant vapor must account for density changes when:

M = V/c > 0.3 (Mach number)

Or pressure drop exceeds:

ΔP/P > 0.1

Compressible Flow Applications:

  • High-velocity duct systems (>4,000 fpm)
  • Refrigerant suction lines (high Mach number)
  • Steam systems above 50 psig
  • Air compressor discharge lines

Property Determination Methods

For Liquids (Water, Glycols)

  1. Reference Tables: ASHRAE Fundamentals Chapter 34
  2. Polynomial Correlations: Curve-fit equations for temperature dependency
  3. Manufacturer Data: Glycol concentration effects (Dow, MEGlobal)
  4. Software: REFPROP, Engineering Equation Solver (EES)

For Gases (Air, Refrigerant Vapor)

  1. Ideal Gas Law: Accurate for air at HVAC conditions
  2. Real Gas Equations: Benedict-Webb-Rubin for refrigerants
  3. Psychrometric Charts: Air-water vapor mixtures
  4. REFPROP Database: NIST-certified properties

For Refrigerants

  1. ASHRAE Standard 34: Refrigerant designation and safety classification
  2. REFPROP 10.0: Reference fluid properties database
  3. Martin-Hou Equation of State: Industrial refrigerant calculations
  4. Manufacturer Software: Refrigerant property calculators

Design Considerations

Fluid Selection Criteria

PropertyWaterGlycol SolutionsRefrigerantsAir
Heat CapacityExcellentGood (20% penalty)FairPoor
DensityHighHighVariableVery Low
ViscosityLowModerate-HighLowVery Low
ToxicityNoneLow (propylene)Varies by classNone
FlammabilityNoneLowVaries by classSupports combustion
CostLowestModerateHighFree

Temperature-Dependent Property Effects

  1. Hot Water Systems (140-200°F):

    • Reduced density (2-4% lower than 60°F)
    • Significantly lower viscosity (60-70% reduction)
    • Higher vapor pressure (requires system pressurization)
    • Expansion tank sizing critical
  2. Chilled Water Systems (40-55°F):

    • Increased viscosity (40-60% higher than 60°F)
    • Higher density (slight increase)
    • Condensation risk at pipe surfaces
    • Glycol addition impacts all properties
  3. Glycol Solutions:

    • All properties degrade compared to water
    • Pumping power increases 30-80% for 30-50% concentrations
    • Heat transfer penalty 5-15%
    • Freeze protection vs. performance tradeoff

Altitude Corrections

Air density at altitude affects:

Fan Performance:

  • BHP_altitude = BHP_std · (ρ_altitude/ρ_std)
  • Pressure developed remains constant (in inches w.c.)
  • Motor may be oversized at altitude

Heat Transfer:

  • Reduced mass flow for same volumetric flow
  • Sensible capacity proportional to density
  • Coil face velocity correction required

Burner Performance:

  • Reduced oxygen availability
  • Deration factors for gas-fired equipment
  • Combustion air fan sizing critical

Pressure Drop Implications

Property effects on pressure drop (Darcy-Weisbach):

ΔP = f · (L/D) · (ρ·V²/2)

Where f depends on Reynolds number:

Re = (ρ·V·D)/μ = (V·D)/ν

Key Relationships:

  1. Pressure drop proportional to density
  2. Friction factor inversely related to Reynolds number (in laminar flow)
  3. Viscosity increase substantially raises pumping power
  4. Temperature changes affect both ρ and μ simultaneously

Best Practices

  1. Use actual fluid properties at operating conditions - not handbook values at 60°F
  2. Account for glycol concentration effects - particularly viscosity and heat capacity
  3. Verify altitude corrections for fan and burner selections above 1,000 ft
  4. Calculate NPSH margin - maintain at least 5 ft above pump requirement
  5. Consider temperature cycling - expansion/contraction in system design
  6. Update properties in energy models - seasonal variations affect performance
  7. Document fluid specifications - concentration, additives, inhibitors
  8. Test actual fluid properties - particularly in critical applications
  9. Account for degradation - glycol breakdown, refrigerant contamination
  10. Reference current ASHRAE data - properties updated with research

Code and Standard References

  • ASHRAE Handbook - Fundamentals: Chapters 1, 33, 34 (Property data)
  • ASHRAE Standard 34: Refrigerant designation and safety
  • ASHRAE Standard 12: Legionellosis risk minimization
  • NIST REFPROP: Thermophysical property database
  • Hydraulic Institute Standards: Pump NPSH requirements
  • SMACNA HVAC Systems Duct Design: Air property applications
  • ASME B31.9: Building services piping (pressure-temperature ratings)