- What is your measured value?
- Choose which number you have. If the amplifier already shows a strain in µm/m (micrometres per metre; 1000 µm/m = 0.1 % change of length), choose strain. If it only shows the raw Wheatstone-bridge signal in mV/V (millivolts of output per volt of excitation), choose signal; gauge factor and bridge circuit are then needed for the conversion.
- Measured strain at 45° ε₄₅ [µm/m]
- The strain shown by a gauge bonded at mid-web at 45° to the force direction. At +45° it is positive (tension), at −45° equally large and negative (compression) – the hallmark of pure shear. For half or full bridges enter the strain of one single gauge. Source: the amplifier reading after zero balancing with the beam unloaded.
- Bridge signal U_M/U_B [mV/V]
- The raw bridge signal: Wheatstone-bridge output divided by the excitation, in mV/V. Keil's shear beam is designed for 1.74 mV/V at 30 kN (before excitation temperature compensation). 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
- 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. One gauge: B = 1. One pair +45°/−45° in adjacent arms: the opposite strains add, B = 2. One pair on each web face (Keil's shear beam, eq. 10.43): B = 4, plus temperature and bending compensation. Source: your own wiring or datasheet.
- Web area
- How the web area is determined: from web height times web thickness, or entered directly (e.g. from the drawing if the web is not rectangular). Meant is only the thin part of the section standing along the force that carries the shear – not the flanges.
- Web height h [mm]
- The web height in the direction of the shear force, i.e. the distance between the two flanges or the height of the shear diaphragm (Keil: 46 mm). Source: drawing or measurement at the milled pocket.
- Web thickness b [mm]
- The web thickness, i.e. the remaining wall between the two milled pockets on whose floor the gauges are bonded (Keil: 4.6 mm). The thinner, the larger the strain for the same force. Source: drawing or measurement.
- Web area A_web [mm²]
- The web area directly in mm², only when ‘enter directly’ is selected. Keil's example: 215 mm² (46 × 4.66 mm rounded). For rolled sections: web height between the flanges times web thickness from the section table.
- 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.