Picture a 37 kW extract fan running 6,000 hours a year with its outlet damper half closed. At the maintenance budget meeting, the proposal on the table is to upgrade the motor from IE3 to IE4. Run the numbers and the picture shifts: the better motor class saves a few thousand kWh a year, while opening the damper and letting the fan run at the speed the process actually needs can save more than ten times that on the very same motor. Most energy programmes start with the motor, yet most of the losses sit in front of it and behind it.
It helps to treat energy as a chain: the supply, the motor, the transmission, the driven machine and, at the end, the work the process really asks for. Each link loses a different amount, and each costs a different amount to fix. The sections below work through the chain starting where the largest gain usually hides.
Measure first: which motors make up the bill?
Knowing how many motors a site has is not the same as knowing which ones drive the electricity bill. A simple list is enough to start: rated power, annual running hours and the running current measured with a clamp meter. Comparing measured current with nameplate current gives a rough load factor, and multiplying the three gives a usable priority score. A 45 kW fire pump that runs 300 hours a year drops to the bottom; an 11 kW cooling tower fan running three shifts climbs near the top.
Without that list, attention goes to the most visible motor, which is usually the largest, loudest or oldest one. Once the list exists, it tends to show that a handful of continuously running pumps, fans and compressors account for most of the consumption. To estimate how loaded a motor really is, see our article on motor load ratio and correct sizing.
The biggest loss is in the process itself
When flow is controlled by throttling a pump valve or closing a fan damper, the motor keeps running at full speed and the surplus pressure is burned off across the valve as heat. For centrifugal pumps and fans, power varies roughly with the cube of speed. Cutting speed to 80% ideally cuts the required power to about half (0.8³ ≈ 0.51). A system with a high static head will show a smaller gain, but in most ventilation and circulation duties the saving is still large.
Back to the opening example. Suppose that for half the year, 3,000 hours, 80% of the airflow would be enough, and the fan draws about 29.6 kW at the shaft. Running it at 80% speed on a variable frequency drive instead of throttling it saves, on paper, 3,000 × 29.6 × 0.49 ≈ 43,500 kWh. Drive losses and the real system curve will reduce that figure, but it remains far above anything a motor class change can offer. The calculation is covered in detail in VFDs, pumps, fans and the affinity laws.
Two related habits are easy to miss. Conveyors left running through breaks, mixers turning while they wait for product and compressors idling unloaded all keep drawing magnetising and friction power; a timer or a level signal that stops them usually costs next to nothing. Set points that are higher than needed, such as a compressed air network running a bar or two above requirement, keep motors running longer and harder.
One caution: the cube law applies to centrifugal loads. On constant-torque machines such as conveyors, reducing speed lowers power only in proportion to speed.
Power lost between motor and machine
- Belts: a slack V-belt slips and heats up; an over-tensioned one loads the bearings.
- Couplings: misalignment adds friction and wears bearings early.
- Gearboxes: worm gear efficiency falls noticeably as the ratio increases. On a continuously running drive, the gap between a high-ratio worm unit and a helical gearbox can be larger than the gap between two motor efficiency classes, so check the efficiency figure in the model table, not just the ratio.
Where a belt-driven fan simply runs faster than it ever needs to, correcting the pulley ratio can be cheaper than adding a drive. Worked examples are in our guide to speed adjustment with pulleys and belts.
The motor's own losses
Three questions matter on the motor side. The first is the efficiency class. Under IEC 60034-30-1, the minimum efficiency of a 4-pole 37 kW motor is 93.9% for IE3, 95.2% for IE4 and 96.1% for IE5. In the fan example, with about 29.6 kW at the shaft, moving from IE3 to IE4 lowers input power by roughly 0.43 kW on a full-load efficiency estimate, around 2,600 kWh over 6,000 hours. That is worthwhile on a motor that never stops, but modest next to the process opportunity. Our article on when to stay with IE3 instead of IE4 works out the payback against running hours.
The second is load factor. Induction motor efficiency stays fairly flat above about half load but falls off clearly at very light load, and power factor gets worse too. Downsizing a large motor running at 30% load improves both; trying to downsize one that runs at 70% usually adds risk rather than savings.
The third is history. A motor that has been rewound several times, especially if the core was overheated during stripping, may have higher losses than when it was new. For bringing energy into the repair decision, see rewind the motor or buy new.











