Strain gauges · Measurement

Shaft Torque from Strain Calculator

Calculate shear stress and shaft torque from the strain measured with 45° gauges or directly from the bridge signal in mV/V.

DMSKeil 2017
01

Inputs

Pure torsion of a circular or annular section without notches at the gauge location; superimposed bending or axial force is rejected only by the full bridge with two opposite pairs. Linear-elastic; temperature response and lead resistance not included.

02

Results

Enter values and run the calculation.

Method

What is calculated?

In pure torsion the shaft surface carries principal normal stresses at ±45° to the axis equal in magnitude to the shear stress; a gauge at 45° therefore measures ε₄₅ = τ(1+ν)/E. This relation can be inverted: the measured strain gives the shear stress, and the polar section modulus gives the torque. Keil's example run backwards: 1054 µm/m on a 24/14 mm hollow shaft with E = 206 000 N/mm² gives τ ≈ 167 N/mm² and M_t ≈ 400 N·m.

Equations

ε₄₅ = 4·(U_M/U_B)/(k·B) (Keil Gl. 4.8, nur Modus Signal)

τ = ε₄₅·E/(1+ν) (Umkehrung von Keil Gl. 10.38)

W_p = π/(16·d_a)·(d_a⁴ − d_i⁴) (Keil Gl. 10.36)

M_t = τ·W_p (Umkehrung von Keil Gl. 10.35)

Limits

Assumptions and typical mistake

Pure torsion of a circular or annular section without notches at the gauge location; superimposed bending or axial force is rejected only by the full bridge with two opposite pairs. Linear-elastic; temperature response and lead resistance not included.

Entering a strain measured along the shaft – it is zero in pure torsion and yields no torque; or choosing the wrong bridge factor in signal mode (a factor-of-2 or -4 error).

Gauge layout

Where the gauges sit and what the bridge makes of them

One card per selectable circuit, in the order of the selector above: first, where the grids sit on the part and in which direction they are strained, then the Wheatstone bridge with Keil's arm occupancy – strains in opposite arms add, strains in adjacent arms cancel.

What does the bridge factor B mean?

The general bridge equation is U_M/U_B = k/4·(ε₁ − ε₂ + ε₃ − ε₄): strains in opposite arms count positive, in adjacent arms negative. Expressing every active strain as a multiple of one reference strain ε, B is exactly that signed sum of multiples – e.g. B = 2 for two adding contributions, B = 4 for four. U_M/U_B = k·B·ε/4 summarises this.

To assess it: B is a pure gain of the circuit, not a statement about temperature compensation or which load type is in the signal – that is covered by “Use” and the response chips below. A larger B gives a larger, more easily measured signal U_M for the same mechanical strain; this calculator inserts B into the calculation automatically once you pick a circuit, so you never enter it yourself.

Full bridge torsion: 2 gauge pairs at ±45° B = 4

Layout: Two perpendicular gauge pairs at 45° to the shaft axis, 180° apart around the circumference; the two gauges of a pair sit in adjacent arms.

1234U_MU_MU_BU_B
  • F compensated
  • M_b compensated
  • M_t in the signal
  • ΔT compensated

Use: The ideal arrangement for measuring torque.

  • All four magnitudes of the 45° principal strains add.
  • Insensitive to axial force, bending and temperature: both gauges of a pair are loaded alike and cancel.
  • Exact 45° alignment required; suppliers offer twin-grid (“herringbone”) gauges for it.
  • On rotating shafts signal transmission (slip ring, telemetry) is required.

Keil Abb. 4.16, Gl. 4.18; Abschn. 10.2.3

Half bridge torsion: 1 gauge pair at ±45° B = 2

Layout: One perpendicular gauge pair at ±45° to the shaft axis at one spot of the circumference, in adjacent bridge arms; two fixed resistors complete the bridge.

12RRU_MU_MU_BU_BR = fixed resistor
  • F compensated
  • M_b compensated
  • M_t in the signal
  • ΔT compensated

Use: When only one spot of the circumference is accessible or a single twin-grid gauge suffices.

  • One twin-grid gauge suffices; temperature, axial force and bending cancel within the pair.
  • Half the signal of the full bridge.
  • Asymmetric layout: bending is compensated only if both grids see the same bending strain.

Keil Abschn. 10.2.3

Quarter bridge: 1 longitudinal gauge B = 1

Layout: One longitudinal gauge on the part; the other three bridge arms are fixed resistors in the instrument.

1RRRU_MU_MU_BU_BR = fixed resistor
  • F in the signal
  • M_b in the signal
  • M_t insensitive
  • ΔT not compensated

Use: Only at constant temperature and for a known uniaxial stress state along the principal direction.

  • Simplest installation, one gauge only.
  • Smallest measuring spot.
  • Temperature response enters the result additively – even with a four-wire connection.
  • Axial force and bending appear together in the signal.

Keil Abb. 4.8, Gl. 4.10

Bridge wiring diagrams after Keil, Dehnungsmessstreifen, 2nd ed. 2017 (secs. 4.5, 9.7, 10.2, 10.5) · bridge arms numbered R1–R4 with U_M/U_B = k/4·(ε₁ − ε₂ + ε₃ − ε₄).
Inputs

What you enter – and where the values come from

What is your measured value?
Choose which number you have. Modern amplifiers in strain-gauge mode display a strain directly in µm/m (micrometres per metre, 1000 µm/m = 0.1 % change of length) – then choose strain. If the instrument only shows the raw Wheatstone-bridge signal in mV/V (millivolts of output per volt of excitation), choose signal; the calculator then also needs the gauge factor and bridge circuit.
Measured strain at 45° ε₄₅ [µm/m]
The strain shown by a strain gauge bonded at 45° to the shaft axis. For a full bridge of two pairs this is the strain of one single gauge, not the sum. Positive when the gauge lies in the tensile direction; the sign gives the direction of the torque. Source: the amplifier reading after zero balancing with the shaft unloaded.
Bridge signal U_M/U_B [mV/V]
The raw bridge signal: Wheatstone-bridge output voltage divided by the excitation, in mV/V. A torque transducer typically gives 1–2 mV/V at rated torque. Source: the amplifier reading in mV/V mode after zero balancing.
Gauge factor k
The gauge factor is the sensitivity of the strain gauge: it states how much the electrical resistance changes when the gauge is stretched (ΔR/R = k·ε). Without it no strain can be computed from an electrical signal. Source: printed on every gauge package or in the manufacturer datasheet, typically 2.0 to 2.1 for constantan foil gauges; valid at room temperature. The same value must be set in the amplifier.
Bridge circuit (signal mode only)
How the 45° gauges are wired – this sets the bridge factor B, i.e. how many times the strain of one gauge is contained in the signal: 1 gauge = B 1, one pair (+45°/−45°) in a half bridge = B 2, two opposite pairs in a full bridge = B 4. Relevant only in signal mode. Source: your own wiring or the measuring shaft's datasheet.
Outer diameter d_a [mm]
The shaft's outer diameter exactly where the gauges are bonded. It enters the torque to the third power – a 1 % error in diameter is a 3 % error in torque. Source: calliper or drawing.
Inner diameter d_i (0 = solid) [mm]
The bore diameter if the shaft is hollow; enter 0 for a solid shaft. A bore removes material that carries little in torsion anyway (the centre is almost stress-free), so it changes the torque less than the outer diameter does. Source: drawing or a measurement at the end face.
Young's modulus E [N/mm²]
Young's modulus describes how stiff the part's material is – how much stress it takes to produce a given strain (σ = E·ε). It is needed to turn measured or computed strains into stresses and vice versa. Source: material tables or datasheet; steel ≈ 210 000 N/mm², aluminium ≈ 70 000 N/mm², titanium ≈ 110 000 N/mm². E drops at elevated temperature.
Poisson's ratio ν
Poisson's ratio states how much a material contracts transversely when stretched longitudinally: ε_transverse = −ν·ε_longitudinal. It matters because transversely bonded gauges measure exactly this contraction and because both directions interact in biaxial stress states. Source: material tables; steel 0.28–0.30, aluminium 0.33, plastics 0.35–0.45.
Context

What this calculator is for

Retrofit torque measurement on drive and gearbox shafts, test-rig evaluation, calibration checks of torque-measuring shafts and determination of the actual service load when only a strain signal is available.

What comes next

  1. Install gauges at 45° to the shaft axis and balance the bridge with the shaft unloaded.
  2. Under load, read the strain (or the mV/V signal) and enter it here; choose the matching mode.
  3. Enter the diameters at the gauge location and the material data; compare the resulting M_t with the allowable or expected torque.
Results

How to read the results

  • The calculator works backwards: from what you measure (strain or signal) to what you want to know (torque). The intermediate shear stress is at the same time the value for the strength comparison.
  • The sign of the torque follows the sign of the strain – which direction of rotation is positive depends on which gauge of the full bridge sits in arm 1; check once with a known rotation direction if needed.
  • "Torque per 1 µm/m" is the conversion number for all further readings from the same measuring point as long as diameter and material stay the same.
Result quantities

What each value means

Strain at 45° used [µm/m]
The strain of one single 45° gauge used in the calculation – in strain mode your entered value, in signal mode the strain converted from mV/V, gauge factor and bridge factor. Lets you check the bridge factor was chosen correctly.
Surface shear stress τ [N/mm²]
The shear stress at the shaft surface that produced this strain. Compare with the material's allowable torsional stress (e.g. τ_allow from Roloff/Matek, or a safety factor against yield).
Polar section modulus W_p [mm³]
The polar section modulus of the section – a pure geometry figure linking shear stress and torque. The larger it is, the more torque the same stress represents.
Torque M_t [N·m]
The torque the shaft actually transmits at the gauge location – the calculator's real answer. Sign as the strain. Compare with the drive's rated torque or the allowable torque; multiply by speed for power (P = 2π·n·M_t/60).
Torque per 1 µm/m [N·m]
The sensitivity of the measuring point: this much torque corresponds to 1 µm/m of strain. Handy as a calibration factor for the amplifier or for quick mental conversion of further readings.
Source

Technical basis

Keil, Dehnungsmessstreifen, 2nd ed. 2017, sec. 10.2.3 torsionally loaded objects, eqs. (10.35)–(10.41); sec. 4.2, eq. (4.8); sec. 9.4, eq. (9.25).

The source supports the equation structure and worked examples; this calculator does not replace calibration of the measuring chain.

FAQ

Frequently asked questions

Why ε₄₅ rather than the strain along the shaft?

In pure torsion the longitudinal strain is zero; the deformation appears only at 45° as tensile and compressive strain of equal magnitude.

Can I derive the power from it?

Yes: P = 2π·n·M_t/60 with the speed n in rpm (see the mechanical-power calculator).

What if bending acts as well?

Two opposite 45° pairs in a full bridge cancel bending and axial force; with a single pair or gauge those components enter the result.