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# The Versatile Strain Gauge Load Cell

## Preface

In load measurement applications, strain gauge load cells are a popular choice. Strain gauge type load cells are cost-effective, accurate and highly configurable. This article explains the underlying technology behind these versatile devices.

## What is a Strain Gauge?

A bonded strain gauge consists of a thin wire etched in a back-and-forth pattern onto a non-conductive substrate material with connectors at each end of the wire (Figure 1). The length of wire is the total length of all the loops; the end loops (labeled) are wider to make negligible any change in resistance from the same length of straight wire. Additionally, note the alignment marks indicating the direction of a normal strain (the top and bottom marks in the figure) and an orthogonal one.

From  a circuit standpoint, the wire acts as a resistor. The strain gauge is a function of the elastic properties of the wire. When the wire is stretched, its length increases, its cross section decreases and therefore its resistance goes up. When the wire is compressed, the opposite occurs. An analogy of this is flexible tubing. When stretched, it lengthens and narrows in cross section which restricts the fluid flow compared to the original tube.

The ratio of the change in length of the wire divided by the original length of the wire is known as its mechanical strain. It is expressed as the equation: where is the conventional symbol for strain, is the change in length of the wire and is the original length of the wire.

The relationship between the change in resistance of the strain gauge, and the strain in the etched wire due to an applied load, is approximately linear within the elastic limit of the wire. This relationship is expressed as a ratio known as the gauge factor ( ). This linear relationship is the key to the strain gauge’s operation. The applied load creates a strain which in turn alters the resistance. Consequently, a voltage drop through the strain gauge will change depending on whether the gauge is under load conditions or not. This change in voltage due to a change in applied strain produces a corresponding change in output voltage of a strain gauge load cell.

Unbonded strain gauges also exist but the bonded type are most common and therefore this article focuses on the latter.

## Strain Gauge Load Cell Circuitry

Strain gauges have load limits. The strain on the wire cannot exceed the point where the metal will no longer return to its original length but instead permanently deforms. For most metals, this change is very small. For example, for steel the elastic limit is a strain of 0.001 mm/mm.

The gauge factor tells us the resistance change in a metal is proportional to the strain. For most metals, the gauge factor is around the order of 2. This means for a strain gauge of 100 ohms unloaded, the maximum change in resistance possible within the elastic limit is about 0.2 ohms.

Obviously this resistance change is very small. In fact, if a simple ohm-meter were to measure it, the change in resistance in the strain gauge would be so small that it would fall within the percent error of the meter, and therefore would be imperceptible. To accurately measure this resistance change, a strain gauge load cell employs a simple circuit known as a Wheatstone Bridge.

### The Wheatstone Bridge

A Wheatstone bridge is simply two voltage dividers wired in parallel arms of a circuit with a common voltage source. Figure 2 shows a representation of this circuit.

The input voltage, , is the excitation voltage. The variable resistor at represents the strain gauge. , , , and have equal resistances and has a value of zero under no load. Therefore when the strain gauge bears no load, the voltages at the nodes and are equivalent and the output of the bridge circuit, which is the voltage difference across these two nodes, is zero volts.

What happens when a force or load is applied and is non-zero? Let’s look at the general equation for the voltage at each output node. Recall ohm’s law states that the voltage between two nodes in a series circuit is equal to the current through it multiplied by the total resistance in that path, or more commonly seen as . Rearranging, , the current on the left half of the bridge circuit in Figure 2 is then equal to . The two resistors along this path divide the excitation voltage at . Substituting our expression for current in the left path for in the ohm’s law equation, this voltage at the node is: Similarly, the voltage at the node is: The total output voltage is simply the difference between these two: The reason this setup improves accuracy is that now the voltage drop across the strain gauge is being compared to the voltage drop across a similar resistance for the same excitation voltage, instead of being compared to the much larger excitation voltage itself. That means the change in voltage across the strain gauge will be the same order of magnitude as the comparison voltage and any error will be a fraction of this. Also, any changes in strain due to temperature or other environmental factors will affect all of the resistors in the circuit equally.

### The Quarter, Half, and Full-Bridge Configurations

All Wheatstone bridges have four resistive elements. However in load cell design, the number of those elements that are strain gauges vs non-variable resistors is flexible. If only one of the resistive elements in the bridge is a strain gauge, it is a quarter bridge. If two are strain gauges, it is a half bridge. And in the case where all four resistive elements are strain gauges, the Wheatstone bridge is a full bridge. See Figures 3-5 below.