Linear variable differential transformer displacement transducers ...
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Data Pack E
Linear variable differential transformer displacement transducers Data Sheet (LVDTs) and instrumentation
Introduction The LVDT is a transducer for converting positional information into an electrical signal. It is wound as a transformer with a single primary and two secondaries wound around a cylindrical bobbin. A moveable nickel-iron core is positioned inside the windings, and it is the movement of this core which is measured, (Figure 1).
Figure 2 LVDT input/output waveforms
Drive (input)
Figure 1 Principle of operation
Output (core fully in)
Output (core half in)
Output (core at centre)
To operate the transducer, it is necessary to drive the primary with a sine wave, the output from the secondaries is then monitored and consists of a sine wave with the positional information contained in the amplitude and phase. The output with the core at the centre of the stroke is zero, rising to maximum amplitude at either end of the stroke. The output is in phase with the primary drive at one end of the stroke and in anti-phase at the other end as shown in Figure 2. In a good transducer, the relationship between position and phase/amplitude is linear. In addition to position measurement, LVDTs can be used in other types of transducers; for instance load cells, accelerometers or pressure sensors.
Output (core half out)
Output (core fully out)
232-4049 LVDTs Miniature ac energised Two miniature ac energised LVDT transducers which provide an economically priced solution for displacement sensors with outstanding rugged construction and high performance. Two sizes are offered ±1mm (RS stock no. 646-527) and ±3mm (RS stock no. 646533). However these transducers can be used for displacement measurements up to 8mm in applications where the infinite resolution and repeatability are more important that linearity. They are suitable for most applications of linear measurement and null sensing, having low residual voltage levels. The epoxy bonded construction makes the devices suitable for operation in wet or oily environments, but not suitable for total immersion. The temperature coefficient for zero is stated using a stainless steel armature carrier and measured relative to mild steel.
Features ● Low cost ● Rugged construction ● Short body length ● Large radial clearance in bore ● Good performance.
Figure 3 SM1 and SM3 dimensions
Electrical specification Type RS stock no. Energising voltage Energising frequency (kHz)
SM1
SM2
646-527
646-533
1 to 10V rms 1 to 20
1 to 20
100k
100k
Primary resistance (Ω)
102
69
Primary impedance (Ω) at 1kHz
Calibration load (Ω)
120
135
2kHz
160
240
5kHz
310
560
10kHz
620
1000
20kHz
1300
1700
204
200
Secondary resistance (Ω) Secondary impedance (Ω) at 1kHz
417
295
2kHz
756
450
5kHz
1830
930
10kHz
3646
1880
20kHz
7280
3900
Sensitivity (mV/v/mm typ.) at 1kHz
69
118
2kHz
110
134
5kHz
142
136
10kHz
147
130
20kHz
149
128
14
3.9
Zero phase shift frequency (kHz) Residual voltage at zero (typ.)