Custom Humanoid Actuator Continuous Torque Testing

Estimate winding heat first, then use the protocol below to request measured continuous torque evidence.

Published · Reviewed

Discuss your continuous torque test plan

Continuous torque thermal estimator

Change the operating point for an instant estimate. All defaults are illustrative, unvalidated assumptions.

0.1–500 Nm · constant output load.

0.1–500 RPM · use standstill mode for 0 RPM.

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Default example shown. Enable JavaScript to edit inputs.

Average winding estimate

114.9 °C

Headroom to entered limit

15.1 K

Winding rise relative to entered limitAmbient 25°CLimit 130°C

Less than 20 K of estimated winding headroom. This is a planning flag chosen for this tool, not a standard acceptance threshold.

Next step: Check parameter uncertainty and sensor error; agree a test margin with the supplier before dwelling at this point.

Housing, grease, magnet and drive temperatures, insulation lifetime and sensor uncertainty are unknown. A winding estimate cannot certify S1 duty. See model assumptions and equations.

Basis: star-connected motor · line RMS current · terminal line-to-line resistance at 20°C. Review electrical and fixture inputs below.

Electrical and fixture inputs
Operating mode

Output torque per motor line RMS ampere for sinusoidal commutation, including reducer efficiency. Convert peak-current catalog values first. Range: 0.05–20 Nm/A RMS.

Terminal DC resistance of a balanced star-connected motor; each phase is RLL/2. Other connections are outside this calculator. Range: 0.01–20 Ω.

Air temperature at the test fixture. Range: -20–70 °C.

Use the supplier-approved winding test limit with your margin; an insulation class alone does not set the joint limit. Range: 60–220 °C.

Winding-to-ambient resistance of the complete assembly in its actual mount. No automatic heatsink or potting multiplier is applied. Range: 0.05–10 K/W.

Effective heating time constant fitted at this load and fixture; do not substitute a bare winding time constant. Range: 1–240 min.

Measured or assumed non-copper heat allocated to this thermal node: core, reducer and coupled drive losses. Example 5 W is an assumption. Range: 0–1000 W.

Blank skips the budget check; exceeding it is flagged independently of winding temperature. Range: 1–1000 W.

Blank skips the ratio; a specified peak must be at least the target continuous torque. Range: 0.1–1500 Nm.

Illustrative scenarios — not measured products

Calculation details and test planning

Line current
12.50 A RMS
Copper heat at 20°C
105.47 W
Total hot heat
149.79 W
Heat budget usage
74.90%
Winding-only torque ceiling
37.13 Nm
Continuous / entered peak
33.33%
Mechanical output (not heat)
91.63 W
Time to 95% of predicted rise
89.9 min

Torque ceiling considers only the winding limit. A fitted time constant yields a first-order 95% rise estimate; actual dwell ends only after the agreed measured stabilization criterion and all component checks. Rig selection also requires torque, speed, overload and control stability checks.

View or manually copy the current test plan

Four decisions before accepting continuous torque

  • Match electrical definitions. Current and resistance conventions change calculated heating. Use the three-phase copper-loss basis before comparing suppliers.
  • Specify the complete fixture. The thermal path is a property of the assembled test, including the mount. Motor heat-balance principles explain why a bare motor value does not settle a joint rating.
  • Qualify each limiting component. The winding calculation leaves housing, grease, magnets and drive unverified. A grease laboratory result cannot substitute for dynamic reducer testing.
  • Separate screening from acceptance. An estimate helps choose the test point. A rating needs an agreed physical test procedure and recorded limits; consult the applicable rating standard.
Decision record: what this page can establish
OutputUse nowStill required
Average winding estimateScreen torque, heat and ambient sensitivityCalibrated fixture inputs and measured temperature
Winding-only torque ceilingIdentify a candidate load pointReducer, drive, magnet and current limits
95% rise timePlan initial logging durationMeasured stabilization and observation window
Mechanical output powerStart rig power selectionTorque-speed envelope and overload checks

Prepared by Custom Humanoid Actuator for joint design and sourcing teams. This is a planning guide; measured actuator qualification records must come from the actual test assembly.

Start with the actuator product families and use the sample RFQ package to record the installation boundary alongside the thermal inputs.

Model, equations and uncertainty

This page derives a steady-state, single-node model at constant output torque. It assumes a balanced star winding, sinusoidal line currents, a constant output Kt, constant fixture Rth and user-supplied other heat at this operating point. It ignores saturation, hot-magnet Kt changes and temperature dependence of non-copper losses. These assumptions must be checked before extrapolation. Thermal model background.

Single-node thermal approximationCopper + allocated other heat [W]Average winding node: T and fitted τActual fixture Rth [K/W] → ambient
Single-node thermal approximation. All heat is lumped into one node. It cannot resolve winding hotspots, housing temperature or the separate reducer thermal path.
Reproducible equations used by the estimator
QuantityEquationMeaning / boundary
Line currentI = T / KtKt uses output Nm per line RMS ampere
Copper heat at 20°CP20 = 1.5 I² RLL,20Derived from 3 I² Rphase for balanced star
Hot copper heatPcu(Tw) = P20 [1 + α(Tw − 20)]α = 0.00393 /°C, approximate copper coefficient
Steady heat balanceTw = Tamb + Rth [Pcu(Tw) + Pother]All allocated heat acts on one average winding node
Closed-form temperatureTw = {Tamb + Rth[P20(1 − 20α) + Pother]} / (1 − α P20 Rth)Only finite when denominator > 0; beyond the entered limit is extrapolation
Winding-only torque ceilingTlim = Kt √{max[0, (Tmax − Tamb)/Rth − Pother] / [1.5 RLL,20 (1 + α(Tmax − 20))]}Not a drive, mechanical or standstill hotspot rating
95% rise timet95 = −ln(0.05) τ ≈ 3ττ is a measured effective loaded value, not a bare winding constant

No stable model equilibrium is reported when 1 − α P20 Rth ≤ 0. The mathematical critical torque is Kt / √(1.5 RLL,20 α Rth); it is a model boundary, not a component safety rating. Near this boundary, parameter error strongly amplifies the temperature prediction. The tool withholds non-finite outputs and asks you to lower load or revise cooling.

Vary measured inputs across their uncertainty bounds rather than relying on rounded single values. Recompute at higher ambient, resistance, other heat and Rth and at lower Kt. Where the margin disappears, collect better data or reduce the proposed load; the tool supplies no probabilistic confidence interval.

Relative copper heat from the square of current0.25 P0.5 IPI4 P2 I
Current sensitivity at fixed resistance. Derived from Pcu ∝ I². Doubling current multiplies copper heat by four before temperature feedback; this is a mathematical comparison, not a measured motor curve.

Electrical definitions that prevent false comparisons

Normalize supplier inputs before comparing a torque claim
Supplier quantityRequired normalizationConsequence if unknown
Kt per peak sinusoidal line ampereKt_RMS = √2 × Kt_peak under that stated conventionAsk for line current and output torque at the test point
Phase winding resistanceRLL = 2 Rphase for star connectionDo not enter phase resistance as line-to-line resistance
Cold resistance at a known temperatureR20 = Rmeasured / [1 + α(Tmeasured − 20)]Repeat four-wire measurement with temperature logged
Motor-only torque constantInclude reduction ratio and efficiency at the operating pointObtain joint output calibration
DC bus current / dq currentDo not treat as line RMS without supplier conversionMeasure phase currents or confirm the drive scaling

Torque reversals, varying reducer efficiency and magnetic saturation can make a single constant Kt inadequate. Log actual phase current and output torque during the physical test. The measurement example also shows why transient mechanical and electrical power must be synchronized.

Build a bench that measures the stated claim

Mechanical measurement chainActuator on the actual limb mountTorque transducer + guarded couplingControlled load motor + speed sensing
Mechanical measurement chain. Measure torque and speed at the actuator output. Coupling alignment and a stable load controller matter at low speed; the diagram specifies no universal accuracy class.

Use the actual mounting interface, installation preload and thermal interface material. Guard the rotating shaft, align the coupling and check the weakest continuous and overload torque rating across the mechanical chain. For static holding, a reaction fixture can replace a rotating absorber, but it still needs load measurement and stable current control.

Instrumentation plan: select uncertainty from the claim
ChannelRecordQualification check
Output torque and speedSynchronized time series; zero and drift checksCalibration and range adequate at the actual low-speed point
Line current and voltageCurrent convention, phase balance and drive settingsCapture relevant ripple; verify acquisition bandwidth for the drive
Winding temperatureEmbedded sensor location or hot-resistance methodState sensor lag and average-versus-hotspot limitation
Reducer, housing, magnet/rotor and driveDirect sensors or validated component-specific estimationCompare each with the exact supplier limit
Ambient and mountAir temperature, fixture drawing, cooling and contact detailsSeparate chamber air from local exhaust and fixture temperature
Three independent temperature checksWinding sensor / hot resistanceReducer and drive temperature sensorsAmbient sensor away from exhaust heat
Three independent temperature checks. Log each channel against time, torque and speed. No fixed percentage maps winding temperature to grease or housing temperature.

Set a total uncertainty budget that resolves the smallest claimed thermal margin. Calibration class alone omits mounting, thermal gradients, drift, sampling and repeatability. Do not select a torque transducer or load motor from a fixed multiplier without checking overloads and the operating envelope.

Run a controlled continuous torque test

Evidence before a continuous ratingAgree boundary, limits and stop rulesLoad in steps and log until stableReview limits + uncertainty + repeatability
Evidence before a continuous rating. A long dwell alone is insufficient. Preserve raw logs and stop the test when any agreed limit is reached.
  1. Agree torque, speed, ambient, mount, drive configuration, winding and component limits, stop rules and the definition of stabilization. Select applicable clauses with the test lab; IEC 60034-1:2026 is a rating reference, not an automatic joint certificate.
  2. Check calibration and zero offsets. Measure cold winding resistance and temperature. Record assembly serial number, lubricant specification and firmware.
  3. Apply a lower commissioning load first. Confirm torque control, speed stability and plausible sensor response before increasing to the target point.
  4. Log synchronized torque, speed, current, ambient and all component temperatures. Stop on any agreed limit, sensor fault or unstable load condition.
  5. Evaluate measured temperature trend over the agreed observation window, with ambient stability and uncertainty accounted for. A brief flat reading is insufficient.
  6. After cooling, inspect and repeat at the required ambient, mounting and duty boundaries. Publish raw data, exclusions and the observed limiting component.
Normalized first-order heating, not measured actuator dataFraction of final rise1.003τ5τ
Normalized first-order heating. Illustration from ΔT/ΔTss = 1 − exp(−t/τ). Three fitted time constants gives about 95% of the final rise; it does not prove measured stabilization.

The tool reports a first-order 95% rise time only. If a lab chooses a slope criterion such as 1 K/h, document the source edition, calculation window, sensor resolution and ambient handling in its procedure. This page does not claim to have verified a mandatory clause number or universal dwell time.

Review this test scope with our engineering team

Standstill holding needs its own evidence

Standstill requires an extra testRotating: phase heating moves in timeStandstill: fixed electrical angleMeasure worst phase at several angles
Standstill requires an extra test. For ideal balanced sinusoidal currents, total copper heat can match the equivalent RMS case while phase hotspots differ. There is no universal stall derating percentage.

A humanoid knee holding a crouch can remain at nearly one electrical angle. Even if the ideal sum of phase current squares gives the same total copper heat as an equivalent rotating RMS case, individual phase temperatures can differ. A single-node average cannot locate the hottest slot or end turn.

Use standstill mode to force zero shaft power and review average heating. Then test several electrical angles under controlled holding torque, observe the hottest accessible winding locations, and agree a position-dependent limit where needed. A brake can reduce energized holding time but requires separate holding and release validation. The report makes no universal 19% or 29% stall derating claim.

Cooling choices: performance, cost and maintenance

Cooling change validationChange potting, interface or airflowMeasure complete fixture Rth againUpdate model and repeat hot dwell
Cooling change validation. Material conductivity alone cannot determine winding-to-ambient thermal resistance. Geometry, interfaces, voids and external cooling remain part of the heat path.
Cooling alternatives and the evidence needed to justify a change
OptionPotential benefit / tradeoffMinimum verification
Conductive limb mountUses existing structure; heat can spread to neighboring jointsRetest with real bracket, contact condition and nearby heat sources
Potting or impregnationMay improve an internal path; adds processing and repair difficultyCheck voids, stress and insulation compatibility; remeasure complete Rth
Forced airMay improve external convection; adds noise, fan power and contamination sensitivityTest actual enclosure airflow and fan-failure behavior
Liquid coolingCan move heat away from a dense joint cluster; adds pumps, seals and plumbingVerify coolant boundary, leakage and loss-of-flow response
Reduce energized duty / use a holding brakeCan reduce average heat; changes motion and safety behaviorTest the actual cycle and brake load/release sequence

Do not multiply the entire winding-to-ambient path by a guessed resin or fan factor. If only winding-to-housing resistance changes, the external path may still dominate. Compare alternatives at identical torque, speed and ambient and include the maintenance cost before selecting an option.

Three worked screening scenarios

These are synthetic demonstrations, not customer results or supplier performance data. Each uses 35 Nm, Kt 2.8 Nm/A RMS, terminal R20 0.45 Ω, 25 RPM, 5 W of assumed other heat, a 130°C winding limit and fitted τ of 30 min. Only the stated ambient or Rth changes. Results below are generated by the same model as the tool.

Continuous torque estimator software run showing a 114.9°C winding estimate and 15.1 K headroom for the 35 Nm example
Actual software execution captured on 22 October 2026 using the baseline inputs listed above. Software demonstration only: this is not a measured actuator test, customer result or supplier endorsement.
Illustrative inputs and derived outputs — no physical qualification
ScenarioAmbient / fixture RthAverage winding estimateTotal hot heatInterpretation
35 Nm example25°C / 0.6 K/W114.9°C149.8 WBaseline screen: component limits and uncertainty still needed
Hot ambient example55°C / 0.6 K/W154.8°C166.3 WAbove winding limit: lower load or improve the measured thermal path
Lower Rth example25°C / 0.42 K/W82.2°C136.3 WLower estimate only if 0.42 K/W is measured in this fixture

Scenario 1 — baseline: Enter the 35 Nm example and review current and hot copper heat. The predicted winding value supplies an initial test point, while the unknown reducer and drive temperatures prevent acceptance.

Scenario 2 — hot ambient: Keep the same load and thermal path, raise ambient from 25°C to 55°C and recalculate. Copper feedback raises the final winding temperature by more than the ambient change. Reduce load before a hot-chamber dwell.

Scenario 3 — changed fixture: Keep 25°C ambient but enter Rth 0.42 K/W. The estimate falls; this is a sensitivity study. Measure that resistance in the real limb before crediting any cooling benefit.

Unknowns that can change the decision

Misuse, cost and scenario risks with practical recovery paths
RiskEffect on the decisionMitigation / alternative
Wrong current or resistance definitionLarge heat error before thermal calculations beginNormalize supplier inputs or measure torque/current and terminal resistance
Unmeasured Rth or omitted other heatFalse apparent headroomTreat output as a sensitivity study; fit an instrumented assembly model
Long hold or slow motionAverage heat misses local phase hotspotsTest fixed angles; use a multi-node model if sensors are insufficient
Grease, magnets, electronics or touch surfacesJoint can exceed a component limit below winding TmaxUnknown until measured; obtain exact component limits
Overbuilt rig or cooling solutionUnnecessary sensor, load motor and maintenance costSet uncertainty and operating envelope first; compare quotes on the same test scope
Changed mount, enclosure, drive or dutyOriginal evidence may no longer represent installationRetest the changed boundary or restrict the claim to the tested one

ASTM D6184-22 is useful for a specified lubricant laboratory test, but its results do not predict dynamic-service oil separation. A fixed grease temperature knee or an actuator MTBF cannot be inferred here. ASTM scope and limitations.

System safety and accessible-surface limits require application-specific review. ISO 10218-1:2025 addresses industrial robots within its scope; it does not make this component calculator a humanoid safety assessment.

Record what was actually qualified

Evidence maturity — proposed procurement gates, not mandated sample counts
PhaseRecordDecision supported
Engineering prototypeFixture model, electrical definitions, thermal sweep and sensor placementChoose candidate operating points and identify missing data
Design validationRepeat at installation boundaries with component limits and uncertaintyFreeze the rating for the specified assembly and conditions
Production validationRepeat across agreed lots, tolerances and assembly processesSet acceptance controls; sample count follows risk and variation
Installation or design changeCompare revised mount, drive, lubricant or enclosure with baselineRetain, restrict or requalify the original continuous torque claim

Include failures, interrupted tests and excluded samples. Report the limiting component even when winding temperature is acceptable. Avoid extending a short hot dwell into a lifetime claim; endurance testing is a separate evidence stream.

Minimum supplier evidence checklist

  • Torque-speed point, peak duration, duty cycle and output current definition.
  • Assembly serial numbers, reducer and lubricant specification, drive settings and firmware.
  • Mounting drawing, preload, thermal interfaces, ambient and any active cooling.
  • Raw synchronized torque, speed, phase current and temperature logs, including warm-up and cool-down.
  • Calibration records, sensor locations, uncertainty, stabilization rule and all component stop limits.
  • Observed limiting component, repeatability, failed runs and the conditions under which the claim stops applying.

If fixture Rth, current convention or component limits are missing, send the checklist and request an instrumented pilot test before accepting a continuous rating. Compare compliance evidence and backlash test conditions as separate qualification dimensions.

Organize the recorded logs with the actuator evidence library and return to the engineering resources for the wider sample qualification workflow.

Engineering and sourcing FAQ

Electrical inputs

Which current convention does the calculator use?

Motor line RMS amperes under balanced sinusoidal commutation. Kt must be output torque divided by that current, including the reducer at the operating point. A drive DC bus current or a peak-current Kt cannot be entered directly.

How do I convert a peak-current torque constant?

If the supplier defines torque as Kt_peak times the amplitude of a sinusoidal line current, Kt_RMS equals sqrt(2) times Kt_peak. Confirm the exact convention with the supplier; a dq current definition can use a different scaling.

Why is the copper-loss factor 1.5?

For a balanced star winding, terminal line-to-line resistance is twice one phase resistance. Three equal phase RMS currents give Pcu = 3 I² Rphase = 1.5 I² RLL. This calculator excludes delta windings and other commutation conventions.

Can I enter a resistance measured at room temperature?

Convert it to 20°C first: R20 = Rmeasured / [1 + 0.00393 (Tmeasured − 20)]. Measure winding temperature with resistance, compensate lead resistance, and document uncertainty.

Is mechanical output power part of the heat budget?

No. Shaft power is torque times angular speed and leaves the actuator mechanically. The thermal budget here compares hot copper heat plus the other heat allocated by the user; it does not compare shaft power.

Thermal boundaries

Does selecting standstill automatically derate torque?

No. Standstill fixes speed to zero and shows only an equivalent average copper-heating estimate. Actual phase hotspots depend on electrical angle, geometry and cooling; instrument multiple rotor angles before accepting a holding rating.

Can I use the motor catalog thermal resistance?

Only if it represents the same complete winding-to-ambient path and mounting condition. A bare winding-to-housing value is incomplete. Measure the assembled actuator in its limb bracket or document the missing external path.

Does potting guarantee a fixed temperature reduction?

No. Resin conductivity, contact area, impregnation quality, voids and external cooling interact. Measure the complete thermal path after the change; this tool applies no automatic potting credit.

Does a winding estimate also predict grease temperature?

No. Reducer losses and thermal paths need separate sensors or a validated multi-node model. Housing, grease, magnet and drive temperatures remain unknown in this tool.

Does a 10 K temperature change predict insulation lifetime?

A general aging rule cannot establish actuator life or MTBF. Insulation-system endurance data, stress profile and other failure modes are required. This page provides no lifespan multiplier or service-life guarantee.

Test execution

Is three time constants a pass criterion?

No. A fitted first-order model reaches about 95% of its final rise at three time constants. Establish the actual stabilization slope, observation window and all component limits in the agreed test procedure.

What does no stable model equilibrium mean?

The copper-feedback denominator is zero or negative, so this linear model has no finite steady-state solution. Reduce current or thermal resistance. The calculator withholds temperature and dwell outputs rather than interpreting infinity as a physical temperature.

How should the load motor be selected?

Check the operating torque-speed envelope, continuous mechanical power, low-speed torque control, overload torque, coupling limits and thermal rating. The calculated shaft watts alone are insufficient for rig selection, especially near zero speed.

What sensor accuracy class is mandatory?

There is no universal class specified by this page. Set the total allowed measurement uncertainty relative to the smallest claimed margin, then include calibration, drift, mounting and acquisition errors for the complete measurement chain.

Does ASTM D6184 define a reducer grease limit?

No. It is an oil-separation laboratory test, and ASTM excludes predicting dynamic-service separation from its results. Use the exact lubricant and reducer supplier limits and measure the actual test assembly.

Supplier decisions

Can a supplier quote continuous torque as a fraction of peak?

A fraction alone does not establish a rating. Request torque, speed, ambient, mounting, thermal logs and limiting component for the tested operating point. Peak duration and recovery conditions should be specified separately.

What happens when I leave optional fields blank?

The winding estimate remains available. Heat-budget usage and the continuous-to-peak ratio are marked not specified. Required fields must contain finite numbers inside the stated ranges.

What if clipboard access is blocked?

Open the current test-plan text beneath the copy button, select it and copy manually. The text includes assumptions, unavailable outputs and next steps; no data is sent automatically.

Can repeated motion be reduced to RMS torque?

RMS torque is a first screen when torque is proportional to current and cycle time is short relative to the relevant thermal dynamics. Long holds, varying efficiency, different speeds and load reversals require time-resolved current and temperature testing.

What is the minimum useful supplier evidence package?

Ask for the actual fixture drawing, electrical definitions, time-series torque/speed/current and temperature logs, sensor calibration, agreed limit criteria and the observed limiting component. Retest when the mount, drive or cooling changes.

Discuss your actuator torque test plan

Bring the estimator summary and the evidence checklist to the engineering discussion. Identify assumed inputs before agreeing a test scope.

Inquiry Email

[email protected]

Include target torque/speed, quantity, and delivery location.

Application Engineer

+8618857971991

Talk directly about drawings, torque-speed targets, and RFQ data gaps.

Or submit detailed CAD/specifications via our technical inquiry form →

Sources, editions and limits of the evidence

Public publisher pages and the engineering references below were checked on . Full licensed standards clauses were not independently audited. Equations and scenario outputs are our stated model derivations; they are not published actuator measurements. Recheck applicable editions when writing a test contract.