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Strain Gauges and Load Cells by the Numbers
Elasticity, resistance, bridges, spring elements, installation, calibration and accuracy for the sensors that weigh and measure force
How strain gauges turn stretch into resistance and how load cells, bridges and weighing systems are designed, installed, calibrated and kept accurate, worked with numbers.
Start readingAbout this book
A load cell is a piece of steel that bends very slightly under load, with four small metal-foil resistors glued to it. When the steel strains, the foil strains with it and its resistance changes by a fraction of an ohm. A bridge circuit turns that change into a few millivolts, and an indicator turns the millivolts into kilograms. Almost every scale, weighbridge, batch hopper, force tester, press monitor and torque transducer in a factory works this way, and almost every weighing problem in a factory comes from forgetting one link in that chain.
This book follows the chain from the atoms up. It starts with why steel springs back and why a metal’s resistance changes when it is stretched, which explains what a strain gauge can and cannot measure and why temperature is its main enemy. It then works through the Wheatstone bridge, the spring elements inside load cells, shear and torque, the installation of a weighing vessel, calibration, accuracy classes and the faults that make a good scale drift.
It is for mechanical, process, maintenance and quality engineers, instrument technicians and plant managers. It assumes engineering or trade training and comfort with stress, strain and simple algebra; the physics is explained as it is used. Each chapter works the running case with real numbers, includes one plausible mistake and how it was found, links the KEVOS® tools that do the chapter’s calculations, and ends with an exercise and its worked answer.
The running case
Every chapter follows one weighing system. This is an illustration. A stock-feed mill in Toowoomba, Queensland, makes mash and pelleted feed for cattle, pigs and poultry. Each batch of up to 2,500 kg of ingredients is weighed in a batch weigh hopper, called BH-2 in this book, before it drops into the mixer.
- Hopper: a steel hopper with a cylindrical upper section 1,800 mm in diameter and 1,200 mm high and a cone tapering to a 300 mm outlet over 1,300 mm. Empty, with its discharge gate and vibrator, it weighs 1,150 kg.
- Load cells: three single-ended shear beam load cells, one under each of the hopper’s three lugs, each rated 2,000 kg, accuracy class C3, rated output 2 mV/V, bridge resistance 350 Ω.
- Support: each load cell sits on a stand of 100 × 100 × 5 mm square hollow section, 2,400 mm tall.
- Electronics: the three load cell cables meet in a junction box on the stand, and a 20 m cable runs to a weighing indicator in the control room, which supplies 10 V excitation and displays in 1 kg steps (0.1 kg in its service mode).
- Below the hopper: a screw feeder driven at 40 rpm by a 5.5 kW geared motor meters the batch into the mixer.
- Test equipment: twenty 25 kg certified test weights, 500 kg in all.
Masses, readings, stresses, prices and failure records are the mill’s working figures or are calculated from stated assumptions. They do not describe KEVOS® work or any real business, load cell maker, instrument maker or supplier. Prices are in Australian dollars excluding GST, because a GST-registered business claims the GST back on its costs.
How to use the book
Chapters 1 to 4 explain the gauge and the bridge, Chapters 5 and 6 the spring elements and multiaxial strain, Chapters 7 and 8 installation and calibration, and Chapters 9 and 10 accuracy and keeping a system honest. Read Chapter 1 first; the others stand on their own once the case is familiar.
Each chapter links the KEVOS® calculators it uses. The tools do the arithmetic; the chapter explains what the inputs mean and where they come from. Every result in the text was checked by calculation, and the numbers in figures match the text.
Limits and responsibility
This book is educational. Weighing systems used for trade must be of an approved pattern and verified under Australia’s trade measurement law, administered by the National Measurement Institute; check the current requirements before using any scale to buy or sell by mass. Hoppers, silos and their supports carry large loads and must be designed and checked by competent engineers to the applicable Australian standards. Electrical work on indicators and junction boxes must be done by licensed people. Datasheet values, readings and costs in the case are illustrations; use the manufacturer’s documents and your own measurements for real work.
Who this book is for
Mechanical, process, maintenance and quality engineers, instrument technicians and plant managers who specify, install, calibrate, troubleshoot or rely on strain gauges, load cells and weighing systems in a factory.
What you will learn
- Explain why a metal springs back, why its electrical resistance changes when it is stretched, and what sets a strain gauge's sensitivity and temperature behaviour.
- Work out the output of quarter, half and full Wheatstone bridges, and find the errors that leads, cables and excitation add to a reading.
- Compare column, bending-beam and shear-beam load cells, and estimate the strain, output and stress of a spring element.
- Install a weighing vessel so that its load cells see only the load, and calibrate it with test weights, substitution and a straight-line check.
- Read a load cell's accuracy class, judge whether a scale is good enough for a tolerance, and detect drift, moisture and fatigue before they cost product.
Inside this book
Chapters
- 01Stress, strain and why steel springs backWhy a metal behaves as a spring, how stress, strain, Young's modulus and Poisson's ratio are related, and why a load cell concentrates strain into a small spring element.
- 02How resistance changes when a conductor stretchesWhy a metal conducts, why its resistance rises when it is stretched, what the gauge factor is made of, how foil and semiconductor gauges differ, and how small the signal from a load cell really is.
- 03Temperature, alloys and apparent strainWhy gauge alloys barely change resistance with temperature, how expansion mismatch causes apparent strain, and how matched gauges, bridges and shielding keep temperature out of readings.
- 04The Wheatstone bridge, leads and excitationHow a Wheatstone bridge turns tiny resistance changes into millivolts, how quarter, half and full bridges compare, and how lead resistance, cable heating and excitation errors are found and removed.
- 05Spring elements: what is inside a load cellHow column, bending-beam, double-bending and shear-beam load cells turn force into strain, how load position affects them, and how to estimate a spring element's strain and stress.
- 06Shear, torque and rosettesWhy gauges at 45° measure shear, how torque transducers work on a shaft, and how a three-gauge rosette gives the principal strains and stresses on a surface whose stress directions are unknown.
- 07Installing a weighing vesselHow to size a hopper's load cells from its volume and load sharing, mount them so the vessel can grow and move freely, and stop pipes, chutes and cables from carrying weight past the cells.
- 08Calibrating with weights and substitutionHow to calibrate a weighing vessel with test weights, substitution and a corner test, judge the result with a straight-line fit, and why datasheet values alone are not enough.
- 09Accuracy classes and whether a scale is good enoughHow to read a load cell's OIML accuracy class and error limits, when trade rules apply, and how a gauge study and error budget show whether a scale can weigh to a tolerance.
- 10Drift, moisture, overload and fatigueHow to keep a weighing system honest between calibrations: daily checks on an EWMA chart, insulation and bridge tests, overload and welding damage, and a fatigue check of the cell.
Apply This in Practice
Use these KEVOS® tools to try the method from this reading with your own numbers.
Applies this method
Axial Stress and Extension
Gives the stress, strain and shortening of a hopper's support leg under its share of a full batch, compared with the much larger strain in a load cell's spring element.
Applies this method
Beam Stress and Deflection
Gives the bending stress and deflection of a cantilever bending-beam load cell, and the stiffness of a rigid pipe that carries weight past a weighing hopper's cells.
Applies this method
Circular Shaft Torsion
Gives the shear stress and twist of a screw feeder shaft under its motor's torque, from which the strain and output of a torque bridge on the shaft are worked out.
Used in Shear, torque and rosettes
Applies this method
Cylindrical Tank Contents
Gives the volume of the cylindrical part of a batch weigh hopper, used with its cone volume to find how much of each ingredient mix the hopper can hold.
Used in Installing a weighing vessel
Applies this method
EWMA Control Chart Check (Weighted Moving Average, Control Limits, Small Shifts)
Charts a weigh hopper's daily test-weight readings as an EWMA and finds the day a slow drift from a damp load cell crosses the control limits.
Applies this method
Fatigue Safety Factor (Goodman)
Checks the fatigue safety factor of a load cell's shear web under the stress cycle of each batch, using equivalent alternating and mean stresses.
Applies this method
Gauge Repeatability and Bias Check (Type 1 Study: Cg, Cgk, Bias t-Test)
Analyses repeated test-weight readings on a batch scale as a Type 1 study, giving Cg, Cgk, bias significance and resolution against an ingredient's tolerance.
Applies this method
Hopper and Frustum Volume
Gives the volume and side angle of a weigh hopper's cone, added to its cylinder to check the batch it holds and the largest load its cells must carry.
Used in Installing a weighing vessel
Applies this method
Linear Calibration Check (Straight-Line Fit, Calibrated Value, Calibration Interval)
Fits a straight line to a weigh hopper's substitution test readings, tests its gain and offset, and gives a reading's calibrated value with its confidence interval.
Applies this method
Principal Stresses and von Mises
Resolves the stresses in a load cell's shear web and from a three-gauge rosette on a hopper lug into principal stresses, their direction and the von Mises stress.
Used in Shear, torque and rosettes
Worked example
Restrained Thermal Stress
Works out the stress and restraint force in a warmed support leg that cannot expand, showing what a temperature-matched strain gauge reads on a free and on a restrained member.
References and source notes
The manuscript and worked examples are original KEVOS® writing. References inform particular concepts; their authors do not endorse this book. Web references were consulted on 2 November 2026.
- A. H. Castro Neto. Elementary Condensed Matter Physics (lecture notes) (2003). Copyright work, used only as a map of ideas: atoms and bonds, crystals, elasticity and dislocations, free electrons in metals, electron scattering by lattice vibrations and by disorder, and semiconductors. No text, equations as set out there, figures or problems are reproduced, and all cases and calculations are KEVOS® originals.
- International Organization of Legal Metrology (OIML). OIML R 60-1:2021 Metrological regulation for load cells, Part 1: Metrological and technical requirements (2021). Read for Chapter 9: the four accuracy classes and their limits on load cell verification intervals, the classification symbol, the maximum permissible errors with the apportioning factor, creep and minimum dead load output return, the temperature range and the humidity classes. Values quoted in Chapter 9 are taken from this edition.
- K. Hoffmann, Hottinger Baldwin Messtechnik. An Introduction to Measurements using Strain Gages (1989). Background for gauge construction, bonding, bridge circuits, lead and cable effects and temperature compensation in Chapters 2 to 4.
- J. W. Dally and W. F. Riley, College House Enterprises. Experimental Stress Analysis, fourth edition (2005). Background for strain gauge sensitivity, rosette analysis and transducer design in Chapters 2, 5 and 6.
- C. S. Smith, Physical Review 94(1), 42–49. Piezoresistance effect in germanium and silicon (1954). Named in Chapter 2 for the discovery of the large piezoresistance of semiconductors on which semiconductor strain gauges rely.
- W. Thomson, Philosophical Transactions of the Royal Society of London 146, 649–751. On the electro-dynamic qualities of metals (1856). Named in Chapter 2 as the early observation that a metal wire's resistance changes when it is stretched.