How a turbocharger works.

Loading the 3D turbocharger 0 of 1.0 MB

The readings, the chart and the guide below already work.

On boost
1.03 bar · 138k rpm
363 Nm · 48 °C
Use two fingers to orbit

Your turbo and engine

Wastegate

Run an experiment

Each runs on the model above from idle, with your frame and engine, and the history scrubber replays it.

History, last 12 snothing yet
Speed
Advanced: engine size, intercooler, altitude, air temperature

The Small and Large frames scale the 3D turbo by their wheel size; engine size and the air change only the numbers.

Results for these settings

Boost
1.03 bar
15.0 psi · PR 2.02
Shaft speed
138k rpm
blade tips 433 m/s
Charge air
48 °C
116 °C out of the compressor
Exhaust
892 °C
drive pressure 0.76 bar, estimate
Wastegate
7° open
22% of the exhaust bypasses
Engine torque
363 Nm
no turbo: 193 Nm, estimate

Live: the machine is running, so after a change these settle within a few seconds.

The compressor map

The dot is the compressor now, and its trail the last 12 seconds (here: Floor it). Lines are shaft speeds; red is surge, dashed is choke (efficiency under 58%).

00.10.20.30.4 11.522.533.5 60%65%70%73%75% 60k80k100k120k140k160k178k Corrected air flow, kg/s Pressure ratio Seconds (the throttle is shaded along the bottom) Boost, bar Shaft, krpm

At the dot

Pressure ratio

2.02

Efficiency

73%

Corrected air flow

0.112 kg/s · 14.8 lb/min

Corrected shaft speed

139k rpm

corrected to 85 °F and 13.95 psia, as maps are drawn

A live 3D turbocharger you can take apart, sized like a real one for a 2.0-litre petrol engine. Exhaust spins the turbine, the turbine drives the compressor on the same shaft, and the compressor stuffs the engine with air. Every reading comes from a model of the turbo's own geometry: open the throttle and watch the lag, watch the wastegate hold the boost, and take the recirculation valve off to make it surge.

How to use the turbocharger simulator

  1. Press Start the turbo, or Take the tour: eight steps that fly the camera round the turbo and run the experiments on it.
  2. Move the throttle and the engine speed on the bar under the model. The readings and the dot on the compressor map move with them, and the "no turbo" figure beside the torque is the same engine without the turbo.
  3. Under Controls, run Floor it to see the lag, or Lift off to see the surge the recirculation valve prevents. Drag the history scrubber back to stop inside either and read what the shaft was doing.
  4. Switch the frame between Small, Mid and Large and run Floor it again: the small turbo comes on boost first and the large one last.
  5. Press Take it apart for a labelled teardown, or open a part in the Learn tab and press Show me. On the model, Space starts and pauses and the arrow keys move the throttle.

Turbine, compressor and the shaft between them

A turbocharger is two turbomachines on one shaft. On the hot side, exhaust leaving the engine at around 890 °C still carries a great deal of energy, and a turbine wheel in its path takes some of it back as shaft work instead of letting it go down the pipe. On the cold side, a compressor wheel on the same shaft draws in air and delivers it to the engine above atmospheric pressure. Between them sits the bearing housing: two floating bronze bearings on films of engine oil, a thrust bearing, and a water jacket, carrying a shaft that turns at up to 178,000 rpm on this frame.

Denser air means more oxygen in every cylinder, so more fuel can be burnt and more torque made from the same swept volume. The no turbo figure beside the torque reading is that proposition as a number: the same engine model with the manifold at the air outside. Wide open at 1,600 rpm, where the turbo has barely begun, the two are close (189 Nm against 177); at 3,500 rpm the boosted engine makes 363 Nm against 193.

The shaft is a power balance, and the simulator solves it thousands of times a second: turbine power minus compressor power minus bearing drag spins the rotor up or down. At steady state the turbine's power equals the other two to within 1%, which the test suite checks. Compressing the air heats it, to 116 °C at 1 bar here, which is what the intercooler undoes before the air reaches the engine. For the theory behind all of it, see turbocharging explained.

Lag, and why frame size is a bargain

Turbo lag is the delay between opening the throttle and getting boost, and it is inertia. The rotor has to be spun from tens of thousands of rpm to well over a hundred thousand, and the only thing spinning it is exhaust energy that doesn't exist until the engine is already making power. Press Floor it and the machine performs the event from idle: on the mid frame boost reaches 0.5 bar 3.5 seconds after the throttle opens. Pull the history scrubber back to stop inside the lag and read what the shaft was doing.

That is why sizing a turbo is a bargain rather than a choice. The small frame has lighter wheels, so it gets to 0.5 bar in 3.3 seconds, but its compressor runs out of flow at high engine speed. The large frame flows far more air at the top and takes 6.0 seconds to get there. The 3D turbo grows and shrinks with the frame, in proportion to its wheels. Modern engines dodge the bargain with twin-scroll housings, variable geometry, two turbos of different sizes, or an electric motor on the shaft.

The wastegate, surge and choke

Left alone, a turbocharger is a runaway: more boost means more fuel and more exhaust, which means more turbine power, which means more boost. The wastegate breaks the loop. Boost pushes on the actuator's diaphragm; once it beats the spring, the rod turns the lever and a flap opens a port that lets exhaust bypass the turbine wheel. On the 1 bar target the flap stands 3° open at 3,000 rpm, passing 12% of the exhaust round the wheel, and 17° open at 6,500 rpm, passing 41%: holding the same boost costs more bypass at higher flow. No wastegate holds the flap shut, and boost runs away to 3.0 bar until the rotor reaches its speed limit 3.6 seconds after the throttle opens.

Surge is the compressor's stall. Shut the throttle on boost and the air in the pipes has nowhere to go while the wheel is still spinning, so the flow through it breaks down and reverses, again and again: here at about 28 times a second, the pipes' own resonance, which is the flutter you can hear. The recirculation valve vents the charge back to the compressor inlet so the flow keeps moving. Lift off does the same lift-off twice, first with the valve removed and then with it fitted: watch the dot cross the red surge line on the first run and stay right of it on the second.

Choke is the opposite wall, on the right of the map. The flow through the wheel's inlet approaches the speed of sound, and extra shaft speed passes little more air: efficiency collapses and the air comes out hot for nothing. The map draws the choke line where efficiency falls below 58%, as turbo makers do. The only fix is a bigger compressor.

Reading a compressor map

A compressor map plots pressure ratio (the air's pressure out over its pressure in) against corrected air flow (the flow scaled to standard inlet conditions, so one map serves every day and every altitude). Each curved line is one shaft speed, in thousands of rpm. The shaded islands are efficiency, best in the middle: the share of the compressor's work that becomes pressure rather than heat. Left of the red surge line the compressor stalls; right of the dashed choke line it runs out of flow.

The dot is the compressor now. At the opening settings it sits at a pressure ratio of 2.02 and 0.112 kg/s, 73% efficient. A well-matched turbo keeps its dot in the islands across the engine's rev range: open the throttle at low revs and it should climb the map without touching surge; hold it wide open to the red line and it should stay left of choke. The map's lines, its surge and choke lines and its islands come from the turbo's wheel sizes and an Euler work estimate fitted to published maps: modelled, not measured.

Frequently Asked Questions

What does "same engine, no turbo" mean on the readings?

It is the torque the very same engine would make with the turbocharger taken off. Both figures come out of one engine model with only the manifold pressure changed — the same displacement, the same volumetric efficiency, the same air–fuel ratio and the same thermal efficiency — so the gap between them is what the turbocharger is buying and nothing else. The one thing deliberately not held constant is charge temperature: boosted air has been through a compressor and an intercooler, while a naturally aspirated engine has neither and breathes air close to ambient, which is denser. Hold the engine wide open at 1,600 rpm and the two numbers are close, because down there the turbine has not yet been given enough exhaust energy to do much; by 3,500 rpm the turbocharged figure is nearly double. That is the honest answer, and it is the point.

Why is the rotor drawn more slowly than it really turns?

Because at true speed you would see nothing. On the mid frame the shaft reaches about 178,000 rpm, roughly 3,000 revolutions a second — at any screen refresh rate that is a featureless grey disc, and worse, it aliases into a wheel that appears to crawl or run backwards. So the rotor is drawn 2,000 times slower than it turns, and the note under the readings on the stage says so, so that nobody counts blade passes and takes the number away as a real one. The physics is not slowed with it: the shaft speed in the readings is the figure the model actually solved, in real time (or at a quarter of it, if you choose ¼×).

How does a turbocharger work?

A turbocharger is two turbomachines on one shaft. Exhaust gas leaving the engine is still hot and still under pressure, and a turbine wheel in its path recovers some of that energy as shaft work. That shaft drives a compressor wheel on the cold side, which forces air into the engine above atmospheric pressure. Denser air means more oxygen per cylinder filling, so more fuel can be burnt and more torque made from the same swept volume.

What causes turbo lag?

Inertia. The rotating assembly — turbine wheel, shaft and compressor wheel — has to be physically accelerated from a few tens of thousands of rpm to well over a hundred thousand, and the only thing accelerating it is exhaust energy the engine cannot produce until it is already making power. Nothing electrical or hydraulic is involved. A lighter, smaller rotating assembly spools faster, which is exactly why small turbos feel responsive and large ones do not.

What does a wastegate do?

It stops the turbo running away. Boost makes more air, which makes more fuel and hotter exhaust, which makes more turbine power, which makes more boost — a loop with no natural limit. The wastegate is a valve that lets exhaust gas bypass the turbine entirely, opening as soon as boost reaches its target and throwing away exactly as much drive as it takes to hold that number. It has to open further at higher engine speed, because the same boost costs more bypass when more gas is flowing.

What is compressor surge and why does it flutter?

Surge is the compressor stalling. It happens when the wheel is asked to hold pressure with too little flow through it — classically the instant a throttle slams shut while the engine is on boost, leaving a plenum full of pressurised air, a closed valve and a wheel still turning at over a hundred thousand rpm. The flow across the blades breaks down and briefly reverses, and the audible flutter is that reversal repeating many times a second. It is hard on the bearings and the wheel.

What is a blow-off or recirculation valve for?

To prevent surge. It opens on a throttle lift and vents the pressurised charge — a recirculation valve returns it to the compressor inlet, a blow-off valve dumps it to atmosphere — so flow keeps passing through the wheel instead of stalling against a closed throttle. Recirculating is the better engineering on a car with a mass-airflow sensor, because air that has already been metered is not thrown away.

What is a compressor map and how do you read it?

A compressor map plots pressure ratio up the side against corrected air flow along the bottom: the flow scaled to standard inlet conditions, so one map serves any weather and any altitude. Curved lines across it are constant shaft speeds; closed contours are islands of equal efficiency. The steep line on the left is the surge line — operating left of it is unstable. The wall on the right is choke, where the flow into the wheel nears the speed of sound and extra shaft speed passes little more air; turbo makers draw it where efficiency falls below 58%. A good match keeps the engine's operating points inside the high-efficiency islands and away from both walls.

Why does boosted air need an intercooler?

Because compressing air heats it. The temperature rise is unavoidable thermodynamics, not friction, and a compressor working at 70% efficiency adds a good deal more heat than the ideal. Hot air is less dense, which throws away part of the density gained by compressing it, and it also makes knock far more likely. An intercooler is a heat exchanger between compressor and engine that removes that heat and hands back most of the density.

Is this simulator using a real compressor map?

Not a maker's map, but not an invented one either. Each frame's wheels are the sizes of a real GT28-class turbo or its neighbours (cited under Sources). The top speed line comes from Euler's work equation at the wheel's tip-speed limit, the choke flow from sonic flow through the wheel's inlet, and the surge line and efficiency islands are shaped the way catalogue maps are; two factors are fitted to published maps, and the code says which. So the map is right in shape and scale, but it is modelled, not measured, and must not be used to size real hardware. Around it runs a transient model with six coupled states on a fixed time step, which the test suite checks against textbook cases and against a power balance that closes to within 1% at steady state.

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