Linear variable differential transformer (LVDT)
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Summary
Introduction
A Linear variable differential transformer, or LVDT, is based on the principles of magnetic induction, the same principle of a "wall-wart" voltage transformer utilized in many electronic device designs. LVDTs are an extremely old position sensing design (> 90 years), partially due to their extremely high precision but also due to their robustness. They also have a high repeatability and accuracy (RDP Group 2002).
An LVDT has four main components:
- Primary coil
- Secondary coil 1
- Secondary coil 2
- Armature
The armature is the moving component whose position is sensed. It is made of a magnetic material. On one side of the armature, the primary coil is excited by a sinusoidal voltage signal, usually 0.5 V – 5 V and between 1 kHz – 30 kHz. This voltage is translated into a variable magnetic field inside the armature. On the other side of the armature, secondary coils 1 and 2 are positioned at some distance. The armature thus induces a current of variable magnatude from the primary coil to each of the secondary ones, varying with its position (RDP Group 2002).
Output
The basic formula which relates transformer coil windings to voltage output is:
<math>\left\frac{Vout}{Vin} \right = \left( \frac{NOut}{NIn} \right)<math>
where N is the number of coil windings and V is the voltage output (eFunda 2005).
Devices
External links & references
- eFunda, 2005, Theory of linear variable differential transformer (LVDT). (http://www.efunda.com/designstandards/sensors/lvdt/lvdt_theory.cfm)
- RDP Group, 2002, LVDT principle of operation. (http://www.rdpe.com/displacement/lvdt/lvdt-principles.htm)
- wikipedia:LVDT
- wikipedia:Transformer
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