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L4 · HVAC Loads and Psychrometrics

Foundation lesson · 25 minute study session

Mix air on a dry-air mass basis

Two air streams combine through conservation of dry air, moisture and energy. A volume fraction is a mass fraction only under suitable density assumptions.

By the end of this lesson

  • Calculate dry-air mass flow from actual airflow and specific volume.
  • Mix enthalpy and humidity ratio independently.
  • Check that a mixed state lies between the inlet states.

Establish flow basis

Psychrometric enthalpy and humidity ratio are expressed per pound of dry air. If actual cfm and specific volume are given, calculate dry-air mass flow for each inlet separately. Equal cfm does not mean equal dry-air mass when the specific volumes differ. Mix hh and WW using m˙da\dot m_{da}, not uncorrected actual volume.

Conserve three quantities

For an adiabatic mixing box with no condensation, dry-air flow leaving equals the inlet total. The outlet enthalpy and humidity ratio are weighted averages using dry-air mass fractions. Read the resulting state from the appropriate chart or property relationship.

Use temperature averaging carefully

A flow-weighted dry-bulb average is a useful approximation when humidity and heat capacities are close. It is not a replacement for the enthalpy and moisture balances when the problem supplies detailed moist-air properties. A mixed state should fall on the straight line between inlet states on a compatible chart.

A decision map for this lesson

Mix properties on the conserved mass basis

The illustration uses the lesson’s adiabatic, no-condensation example. Check those assumptions before applying a simple weighted average.

Conserve dry-air mass through the mixing boxConnect the equipment to the calculation

01 · Equipment view

A realistic cutaway air handler shows outdoor and return inlets joining in a mixing plenum upstream of a coil and fan.

Outdoor air + return air → mixing plenum

For this lesson, isolate the two-inlet mixing plenum. The downstream coil and fan are outside the mixing-box balance.

02 · Exam-style model

Zoom in to read every label.

Conserve dry-air mass through the mixing box

100%Open in a new tab

Scroll or swipe inside the viewport. Read the units and assumptions with the labelled components.

Outdoor air at 1200 pounds dry air per hour and return air at 3600 pounds dry air per hour mix adiabatically without condensation. Outlet flow is 4800, enthalpy 31 and humidity ratio 0.01025.

A 25% outdoor dry-air mass fraction gives the same weights for enthalpy and humidity ratio in this adiabatic, no-condensation example.

Original teaching figure. The schematic and stated givens define the model; the 3D view illustrates the hardware. These are not actual examination exhibits.

Choose the governing relationship and catch the wrong route
Condition or questionGoverning decisionError to avoid
Dry-air mass flows are suppliedUse each dry-air flow divided by their sum as the weight for h and W.Using equal weights when the supplied dry-air flows differ.
Actual cfm and specific volume are suppliedConvert each stream with m˙da=60V˙/v\dot m_{da}=60\dot V/v before weighting hourly flows.Treating equal actual cfm as equal dry-air mass at different specific volumes.
Adiabatic mixing without condensationMixed h and W lie between the corresponding inlet values.Accepting a mixed enthalpy above both inlets without investigating the balance.
A liquid drain or added heat is presentAdd that mass or energy stream to the control-volume balance.Continuing to use the no-condensation, no-heat-input model.

On a narrow screen, scroll across the table to compare the decision and the error.

Relationships and their limits

Convert actual flow

m˙da=60V˙/v\dot m_{da}=60\dot V/v

V is actual ft³/min and v is ft³/lb dry air. Result is lb dry air/h.

Mix the streams

hm=∑m˙da,ihi∑m˙da,i;Wm=∑m˙da,iWi∑m˙da,ih_m=\frac{\sum\dot m_{da,i}h_i}{\sum\dot m_{da,i}};\quad W_m=\frac{\sum\dot m_{da,i}W_i}{\sum\dot m_{da,i}}

Assumes steady, adiabatic mixing, no condensation and a common pressure basis.

Symbols and unit basis
SymbolMeaningUnits or basis
m˙da\dot m_{da}Dry-air mass flowlb dry air/h
V˙\dot VActual volumetric flowcfm
vvSpecific volume per dry-air massft³/lb dry air
hmh_mMixed-air enthalpyBtu/lb dry air
WmW_mMixed-air humidity ratiolb water/lb dry air
hhStream enthalpyBtu/lb dry air
WWStream humidity ratiolb water/lb dry air

One decision, fully worked

Apply the method.

An AHU mixes 1,200 lb dry air/h of outdoor air at h = 40 Btu/lb and W = 0.014 with 3,600 lb dry air/h of return air at h = 28 Btu/lb and W = 0.009. The box is adiabatic and no condensation occurs. Find the mixed h and W.

  1. Add the two dry-air mass flows.
  2. Find the outdoor-air dry-mass fraction, 0.25.
  3. Weight the two enthalpies using the dry-air mass fractions.
  4. Weight the two humidity ratios using the same fractions.
hm=0.25(40)+0.75(28)=31 Btu/lbdah_m=0.25(40)+0.75(28)=31\ \mathrm{Btu/lb_{da}}Wm=0.25(0.014)+0.75(0.009)=0.01025 lbw/lbdaW_m=0.25(0.014)+0.75(0.009)=0.01025\ \mathrm{lb_w/lb_{da}}
Decision

Mixed-air enthalpy is 31 Btu/lb dry air and humidity ratio is 0.01025 lb/lb dry air.

Independent check

Both results lie between the respective inlet values and nearer the return-air state, which supplies 75% of the dry-air mass.

Specialist extension

Equal actual volumes need not be equal mass weights

Mixing balances require a common dry-air mass basis. If stream specific volumes differ, equal actual cfm deliver different dry-air mass rates. For an adiabatic mixer without liquid transfer, mass-weight enthalpy and humidity ratio separately. Use compatible pressure and state definitions; a direct temperature average is not a substitute for the energy balance.

A new applied case

Two streams each deliver 900 actual cfm at a common 14.7 psia. Stream 1 has specific volume 13 ft³/lb dry air and h = 20 Btu/lb dry air; stream 2 has 14 ft³/lb dry air and h = 35. Mixing is steady and adiabatic without condensation. Use the stated vapor-only air states.

m˙1=900(60)/13≈4153.846;m˙2=900(60)/14≈3857.143 lbda/h\dot m_1=900(60)/13\approx4153.846;\quad\dot m_2=900(60)/14\approx3857.143\ \mathrm{lb_{da}/h}hm=(900/13)(20)+(900/14)(35)900/13+900/14=27.222 Btu/lbdah_m=\frac{(900/13)(20)+(900/14)(35)}{900/13+900/14}=27.222\ \mathrm{Btu/lb_{da}}

Decision. Use mixed enthalpy about 27.222 Btu/lb dry air; retain unrounded mass weights.

Cross-check. It lies between the entering enthalpies and closer to stream 1, which has the larger dry-air mass flow. At the stated pressure, the approximate inlet states are 50.1°F with W = 0.00736 and 84.0°F with W = 0.01351; both are below saturation. Check physical state consistency as well as the weighted average.

Unit basis. Specific volume is ft³/lb dry air; actual volume is cfm; dry-air mass rate is lb/h; h is Btu/lb dry air.

NCEES PE Mechanical Reference Handbook v2.1; see the module reference path.

Open targeted practice in the study studio →

Transfer the method

HVAC Loads and Psychrometrics · HV-LC-L4

Try a new decision.

Select one

Two air streams mix steadily and adiabatically without condensation. Stream 1 has 1,000 lb dry air/h, h = 44 Btu/lb dry air and W = 0.016. Stream 2 has 4,000 lb dry air/h, h = 29 and W = 0.006 on matching bases. The mixed-air enthalpy and humidity ratio, respectively are most nearly:

Select one answer

A lesson check supports practice, not a readiness score. Your response stays in this page session and clears on reload.

Catch the common errors

  • Averaging relative humidity directly.
  • Using cfm weights when inlet specific volumes differ materially.
  • Including fan heat in a mixing box explicitly defined as adiabatic.

Handbook navigation drill

Find it, then explain it.

Search: Adiabatic Mixing of Two Moist Airstreams

Find all three balances and identify which mass basis they use.

Check your navigation

You can calculate both outlet h and W without averaging RH.

Reference path: §9.2.1, p. 479; §9.2.3, p. 481. These are printed handbook page numbers; section names and search terms remain the primary navigation method. See technical review status.

Theory sources

  • NCEES handbook v2.1, §9.2.3.
  • Grondzik and Kwok, Mechanical and Electrical Equipment for Buildings, 12th ed., ch. 12, Active Climate Control.

Worked examples and lesson prose are original ReasonSpan™ material. Obtain authorized publications separately; this preview does not reproduce the supplied books or handbook.