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PRESENTATION ON
LVDT
FUNCATION
 An LVDT Displacement Transducer have 3 coils ; a primary
and two secondary's.
 The transfer of current between the primary and the
secondary's of the LVDT displacement transducer is
controlled by the position of a magnetic core called an
armature.
 On our position measurement LVDTs, the two transducer
secondary's are connected in opposition.
 At the centre of the position measurement stroke, the two
secondary voltages of the displacement transducer are
equal but because they are connected in opposition the
resulting output from the sensor is zero.
 As the LVDTs armature moves away from centre, the
result is an increase in one of the position sensor
secondary's and a decrease in the other. This results in
an output from the measurement sensor.
 With LVDTs, the phase of the output (compared with
the excitation phase) enables the electronics to know
which half of the coil the armature is in.
 The strength of the LVDT sensor's principle is that
there is no electrical contact across the transducer
position sensing element which for the user of the
sensor means clean data, infinite resolution and a very
long life.
 Our range of signal conditioning electronics for LVDTs
handles all of the above so that you get an output of
voltage, current or serial data proportional to the
measurement position of the displacement transducer.
CIRCUIT
SECONDARY 1 SECONDARY 2
MATHEMATICAL EQUATION
 Transformer
 The basic transformer formula, which states that the
voltage is proportional to the number of coil windings,
is the backbone of the LVDT. The formula is,
Vout/Vin=Nout/Nin
 where N is the number of coil windings and V is the
voltage read out.
 This equation is,
D=MVout
 where D is displacement of the iron core with respect to
the transformer, and M is the sensitivity of the
transformer (slope of the displacement-voltage curve).
.
 Ratiometric Wiring LVDTAnother commonly used LVDT
wiring is known as ratiometric wiring, as shown
schematically below.
 Ratiometric Wiring
 The displacement for ratiometric LVDT's is given by the
relation,
D=M * VA-VB/VA+VB
Used
Mostly as a sensor in different field

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Power electronic presentation on LVDT

  • 2. FUNCATION  An LVDT Displacement Transducer have 3 coils ; a primary and two secondary's.  The transfer of current between the primary and the secondary's of the LVDT displacement transducer is controlled by the position of a magnetic core called an armature.  On our position measurement LVDTs, the two transducer secondary's are connected in opposition.  At the centre of the position measurement stroke, the two secondary voltages of the displacement transducer are equal but because they are connected in opposition the resulting output from the sensor is zero.
  • 3.  As the LVDTs armature moves away from centre, the result is an increase in one of the position sensor secondary's and a decrease in the other. This results in an output from the measurement sensor.  With LVDTs, the phase of the output (compared with the excitation phase) enables the electronics to know which half of the coil the armature is in.  The strength of the LVDT sensor's principle is that there is no electrical contact across the transducer position sensing element which for the user of the sensor means clean data, infinite resolution and a very long life.  Our range of signal conditioning electronics for LVDTs handles all of the above so that you get an output of voltage, current or serial data proportional to the measurement position of the displacement transducer.
  • 5. MATHEMATICAL EQUATION  Transformer  The basic transformer formula, which states that the voltage is proportional to the number of coil windings, is the backbone of the LVDT. The formula is, Vout/Vin=Nout/Nin  where N is the number of coil windings and V is the voltage read out.  This equation is, D=MVout  where D is displacement of the iron core with respect to the transformer, and M is the sensitivity of the transformer (slope of the displacement-voltage curve).
  • 6. .  Ratiometric Wiring LVDTAnother commonly used LVDT wiring is known as ratiometric wiring, as shown schematically below.  Ratiometric Wiring  The displacement for ratiometric LVDT's is given by the relation, D=M * VA-VB/VA+VB Used Mostly as a sensor in different field