Compressor Sizing & Selection Guide (kW, BTUH, Displacement)

Start from the load, convert it into refrigerant mass flow, then displace that volume at real suction conditions. Here is the arithmetic engineers actually use — how kW, BTU/h and tons fit together, and why the same compressor delivers a different capacity on a hot day.

Updated September 17, 2026 Field Guide 12 min read

Sizing Starts With the Load, Not the Compressor

A compressor is not sized from the room, the pipe size, or the compressor that was there before. It is sized from the load — the heat the system has to remove at design conditions — and then matched to the evaporating and condensing temperatures that the rest of the plant will actually produce. Change either one and the required compressor changes with it.

Build the load first. For a cold room or a process chiller, that means adding every term, not just the obvious one:

The load is the contract

Everything downstream — compressor displacement, condenser surface, pipe size, TXV, electrical supply — follows from the load and the two saturation temperatures. If the load is wrong, a perfectly selected compressor is still the wrong compressor. Write the load down with its assumptions before you open a catalogue.

The Displacement Formula (Swept Volume × Speed)

Once the load is known, the compressor's job is to move enough refrigerant vapour to carry that heat away. The chain is three steps long, and every selection problem is a failure at one of them.

ṁ = Q₀ / Δh₀
mass flow (kg/s) = cooling capacity (kW) ÷ refrigerating effect (kJ/kg)
V̇ = ṁ × v₁
required volumetric flow (m³/s) = mass flow × suction specific volume (m³/kg)
geo = V̇ / ηv = Vd × N / 60
geometric displacement needed = actual flow ÷ volumetric efficiency; Vd is displacement per revolution (m³/rev) and N is speed (rpm)

Reading it in words: the load fixes the mass flow, the suction specific volume converts mass flow into volume flow, and volumetric efficiency — the fraction of the swept volume that is actually delivered as useful vapour after clearance, valve and re-expansion losses — converts volume flow into the hardware you have to buy. Volumetric efficiency is not a constant. It falls as the pressure ratio rises: a compressor that delivers 0.88 at a 2.5:1 ratio may deliver 0.62 at 6:1.

Two numbers in those formulas move more than everything else: v₁ (suction specific volume) and ηv. Both depend on the evaporating temperature and the pressure ratio, which is why you re-check the displacement at the worst condition the plant will see — pull-down, high ambient, or a fouled condenser — and not only at the design point. The compressor selection calculator evaluates exactly these three expressions from CoolProp state data, so you can see how the required displacement grows as the suction pressure falls.

kW, BTU/h and Tons: Getting the Units Right

Most sizing errors we see are not engineering errors, they are unit errors. Cooling capacity in this trade travels in three units, and they are all in daily use: kW (metric design work, Europe and most equipment datasheets), BTU/h (North American equipment, and most residential nameplates), and tons of refrigeration (North American load calculations and legacy drawings).

Unit Equals Where you will meet it
1 kW3,412 BTU/h · 0.2843 tonMetric design loads, EU/Asian equipment datasheets, chiller ratings.
1 ton (TR)3.517 kW · 12,000 BTU/hUS load calculations, split-system nameplates, old drawings.
1 BTU/h0.000293 kWNameplate capacity, small display cases and reach-ins.
1 kW of input power≈ 3.0–3.6 kW of coolingCompressor electrical data at typical air-conditioning conditions.
Conversion is not the same as equivalence: a catalogue rating of 30 kW and a load of 102,000 BTU/h are the same number only if both are stated at the same saturation temperatures. They usually are not.

And do not mix up cooling capacity with input power. A compressor with 7.7 kW of motor input might deliver 30 kW of cooling at one condition and 21 kW at another; the nameplate electrical data tells you what the motor draws, never what the system removes.

Why One Compressor Has Many Capacities

A published compressor capacity is a point, not a property. The number in the catalogue is valid at the standard rating conditions — for EN 12900 / ARI 540 that is 7.2 °C evaporating, 54.4 °C condensing, 8.3 K subcooling and 18.3 °C suction return. Move away from those conditions and the same hardware delivers materially more or less. As a rule of thumb for a scroll or reciprocating compressor in the usual range:

Evaporating / condensing Capacity vs. standard rating Suction specific volume
5 °C / 45 °C1.00 (reference)1.00
10 °C / 45 °C≈ 1.08≈ 0.94
0 °C / 45 °C≈ 0.92≈ 1.07
5 °C / 55 °C≈ 0.87≈ 1.00
0 °C / 55 °C≈ 0.80≈ 1.07
Use the OEM table, not this table

These factors are typical magnitudes for orientation only. They are not a substitute for the manufacturer's performance table or selection software, which accounts for the specific refrigerant, speed, injection and economiser arrangement. When the conditions sit far from standard, always correct with the OEM data — and remember that the compressor's hot-gas and pull-down duty is the sizing case for motor protection, even when the steady-state load is smaller.

Because capacity moves with conditions, a correct selection usually ends with a small table rather than a single number: capacity and required input at design, at pull-down, and at the maximum condensing temperature the plant can see on the hottest day. Add the superheat and subcooling targets from our charging guide to the same sheet and the whole plant is described in one page.

Worked Example: 30 kW (102,000 BTU/h) R-410A System

Take a small industrial chiller: 30 kW of required cooling at 5 °C evaporating and 45 °C condensing, R-410A, 6 K of superheat at the evaporator outlet and 5 K of subcooling at the condenser outlet. Find the mass flow, the required displacement, and a realistic compressor input.

30 kW
Required cooling capacity
102,364
BTU/h (30 × 3,412.14)
8.5
Tons (102,364 ÷ 12,000)

1. Mass flow. The refrigerating effect Δh₀ is the enthalpy difference across the evaporator: suction vapour with 6 K of superheat is about 428.5 kJ/kg, and the liquid arriving at the expansion valve after 5 K of subcooling is about 274.9 kJ/kg, so Δh₀ ≈ 153.6 kJ/kg and

ṁ = 30 / 153.6 = 0.195 kg/s (704 kg/h)
CoolProp state data at the four cycle points; refrigerant properties change with the phase-out, so re-run for R-454B or R-32

2. Volume flow. Saturated R-410A vapour at 5 °C occupies about 0.0280 m³/kg, so

V̇ = 0.195 × 0.0280 = 0.00547 m³/s (19.7 m³/h, 11.6 CFM)
this is the volume the suction side of the compressor must swallow, at suction conditions — not at standard air conditions

3. Geometric displacement. At this pressure ratio a scroll of this size runs around ηv = 0.85, so the swept volume you need is

geo = 0.00547 / 0.85 = 0.00644 m³/s (23.2 m³/h, 13.6 CFM)
at 2,900 rpm that is about 133 cm³ of displacement per revolution — the number you match against a datasheet

4. Input power and check. With an isentropic efficiency of about 0.70, compression from 428.5 kJ/kg to roughly 45 °C condensing costs about 31.5 kJ/kg of ideal work, which is 0.195 × 31.5 ≈ 6.2 kW ideal and about 8.8 kW at the shaft. That gives a cycle COP of 30 / 8.8 ≈ 3.4. The Carnot ceiling at 5 °C / 45 °C is 278.15 / 40 = 6.95, so this machine sits at about 49% of Carnot — a normal figure for a small packaged chiller, and a useful sanity check. If your selection claims 6.0 COP at these temperatures, the state points are wrong somewhere; the COP guide shows how to reconcile the two.

Selection Procedure, Step by Step

  1. Fix the design conditions in writing. Load in kW (and its BTU/h and ton equivalent), evaporating temperature, condensing temperature, subcooling, superheat, refrigerant, and the design ambient that produces them. These are decisions, not outputs.
  2. Convert the load into an enthalpy duty. Pull the four cycle state points for the chosen refrigerant, take Δh₀, and get the mass flow — then the volume flow from the suction specific volume. If the tool and the hand calculation disagree, the state points differ, not the physics.
  3. Add the worst case. Repeat at pull-down and at maximum condensing temperature. The compressor must start and stay inside its envelope at the hardest point, not only at the design point.
  4. Match against real datasheets. Swept volume per revolution and speed give geometric displacement; compare with the OEM performance table at your actual Te/Tc, not at standard rating conditions. Check motor input, current at maximum load, and the operating envelope limits (discharge temperature, pressure ratio, minimum suction superheat).
  5. Record the result as a selection sheet. Capacity, input power, COP, volumetric efficiency assumed, displacement required vs. selected, and the correcting factors you applied. That sheet is what makes the next service call, the next refrigerant change, or the next efficiency upgrade cheap instead of mysterious.
The 30-second check

Capacity (kW) ≈ mass flow (kg/s) × refrigerating effect (kJ/kg), and mass flow ≈ geometric displacement (m³/s) × ηv / suction specific volume (m³/kg). If a proposed compressor cannot deliver that mass flow at the design suction volume, no amount of condenser surface will fix the selection.

Sizing Mistakes and How They Show Up in the Field

These are the failures that survive commissioning and show up as warranty calls. Each one has a signature you can measure, which is the point: sizing mistakes are visible in the cycle, not just on the invoice.

Symptom Likely sizing cause What to check
Short cycling, setpoint reached then a long off cycleCompressor oversized for the real loadPull-down time, cycles per hour, and the real vs. assumed infiltration and product load.
Never reaches setpoint, runs continuouslyUndersized at actual conditionsCompare actual Te/Tc with design — a fouled condenser or low charge steals capacity before the compressor is at fault.
High discharge temperature, oil breakdownPressure ratio outside the envelope, or low suction superheatDischarge line temperature and pressure ratio against the OEM envelope; superheat at design conditions.
Capacity collapses on hot days onlySelected from a standard-condition rating with no correctionRe-read the capacity table at the actual condensing temperature, then re-check the load margin.
Motor trips on pull-down, fine at steady stateSelection made at steady-state load onlyCurrent at maximum load, hot-gas or bypass arrangement, and the envelope limit that the pull-down point crosses.

Every one of these is cheap to catch before purchase and expensive after commissioning. Two habits prevent most of them: keep the design conditions and load assumptions on one page, and re-compute the required displacement at the worst condition the plant will meet. If the cycle ever looks impossible for the hardware — COP above Carnot, or a suction volume the compressor cannot move — the state points are wrong, and the modern alternatives to legacy desktop tools will show you which one.

Start from the load, convert honestly, correct for real conditions, and verify the compressor against its own envelope. That is the entire discipline — the arithmetic is just bookkeeping once the assumptions are on paper.

Size a Compressor in the Browser

The free compressor selection calculator takes your load, suction and discharge conditions, computes the mass flow, required displacement and volumetric efficiency, and shows the cycle on the P-h diagram — CoolProp state data, no install, no licence.

Open the Compressor Sizing Calculator →
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