
Noncontact measurement systems offer several advantages over contact methods. They can be used on small or fragile parts where contacting the target can cause damage. They have higher accuracy and resolution than traditional contact devices and can be used in closed-loop, highly dynamic environments to provide real-time process information and control without operator intervention. Choosing and deploying the correct measurement technology for a control loop is as critical as the measurement itself.

Each noncontact measurement technology has its own set of advantages and disadvantages. Selecting the correct technology often involves a compromise between sensor performance and the environment in which it must operate.
When selecting a measurement technology, an engineer must define the key parameters of the application. The most important parameter to determine is the target material. If the material is not partially electrically conductive, a capacitance or eddy current probe will not work. This can be overcome by adding a conductive material at the measurement site, but this may not be feasible. A fiber optic or laser-based system is then considered.

After the target material, measurement range, accuracy and resolution are specified, the appropriate measurement technology is chosen and the remaining system features determined. Probe geometry is determined and a probe amplifier is selected that suits the required frequency response of the application. Again, this is often a trade-off between system performance and probe size.
In general, the larger the measurement range, the larger the probe size and the lower the absolute system accuracy. It is important not to overspecify the accuracy and resolution required. It may lead to selecting an incorrect system.
While the cost of deploying measurement systems is a concern, it should not carry undue influence when evaluating each measurement technology. Consider the impact of deploying the incorrect solution. The money saved by choosing a given technology can be quickly overshadowed by the cost of incorrect or insufficient measurement.


In its simplest form, an eddy current sensor consists of a precision wire coil around a ferrite core. When an AC current flows through the coil, a magnetic field is formed about the coil. When the coil and its magnetic field are placed in proximity to a conductive target, electric currents are established in the target. These currents, traveling in closed loops opposite the direction of current in the coil, are called eddy currents. The eddy currents, in return, generate their own magnetic field. As the distance between the coil and the target-air gap-is changed, the eddy current magnetic field changes the overall electrical impedance of the sensor coil. The change in coil impedance causes a change in the voltage across the coil, which can be converted to a change in output by the probe amplifier.

Nonlinearity is typically specified as a percentage of full range. For example, a 14-millimeter-range probe with a specified nonlinearity of ±1% field strength will have a maximum displacement error of ±0.14 millimeter. Higher linearity can be achieved using signal processing techniques such as look-up tables.

Environment. Nonconductive mat-erials in the sensor-to-target gap do not affect eddy current sensors. This allows their use in dirty environments-dirt, water, oil and machine fluids-where other displacement sensor technologies fail. However, the presence of conductive materials near the sensor face may distort the magnet field generated by the coil and eddy currents. To minimize the effect of nearby conductive materials, a shielded sensor tip should be used.
Large temperature changes in the measurement area will induce measurement errors. The impedance of the coil and target changes as temperature changes.
Target material. Eddy current displacement sensors require that the target be electrically conductive. The magnitude of the coil impedance change is directly influenced by the resistivity and magnetic permeability of the target material. Ideally, the target is a nonferrous, low-resistance material such as copper, aluminum or brass; however, ferrous material targets can be used.
Systems are frequently calibrated at the manufacturer in accordance to API 670, which specifies the target material to be 4140 stainless steel. For maximum range and accuracy, use target materials with similar electrical resistivity and magnetic permeability to the material for calibration.
Target size. Target size and shape must be considered when selecting an eddy current probe. Target thickness must be at least 1 millimeter. The coil emits a toroidal magnetic field that is approximately three times the diameter of the coil, therefore, the target size should be at least three times the probe tip diameter. When measuring shaft radial runout, the curved surface of the target will distort the magnetic field and limit the full-scale range of the system.
Noncontact displacement measurement is an integral part of process control. Selecting and deploying the correct measurement technology is critical to successfully gathering accurate and reliable data. Eddy current sensors offer a low-cost, high-accuracy solution for many common displacement measurements. Understanding the principles of eddy current probe operation and the parameters that affect their performance is the key to successful deployment. NDT