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Electric transducer
    (Load cell)

      Prepared by: Uday A. Korat
                   (B.E. 3rd year(EC),LDCE)
Electric transducer
• A transducer is a device that converts one
  form of energy to another. Energy types
  include (but are not limited to)
  electrical, mechanical, electromagnetic
  (including light), chemical, acoustic or
  thermal energy.
• Electric transducer: A device which
  converts any kind of energy into electric
  signal whether it is analog or digital.
Types of Electric transducer
• Sound -> Electrical (microphones)

• Force -> Electrical (Load Cells)

• Kinetic -> Electrical
  (piezoelectric, generators)

• Light -> Electrical (solar panels)
• Thermal -> Electrical (thermocouple)
Load cell
• Load cells are integrated sensors that
  measure weights and output continuous
  electrical, pneumatic, or hydraulic analog
  signals.
• A load cell is generally comprised of three
  parts: a mechanical system, a strain
  gauge, and an electronic amplification
  device
• The measurement of a force is done by
  the use of these three parts in the order
  they are listed. It should be noted that load
  cells can be configured with multiple
  "strain gauges".
Strain gauge
• When external forces
  are applied to a
  stationary
  object, stress and
  strain are the result.
• Stress is defined as
Strain gauge
• Strain is defined as the amount of
  deformation per unit length of an object
  when a load is applied.
             Strain (ε) = ΔL/L
• Typical values for strain are less than
  0.005 inch/inch and are often expressed
  in micro-strain units:
             1 μstrain = 106 strain
Strain gauge
• Strain may be compressive or tensile and
  is typically measured by strain gages.
• It was Lord Kelvin who first reported in
  1856 that metallic conductors subjected
  to mechanical strain exhibit a change in
  their electrical resistance.
• This phenomenon was first put to
  practical use in the 1930s.
Strain gauge
• Fundamentally, all strain gages are
  designed to convert mechanical motion
  into an electronic signal.
• A change in capacitance, inductance, or
  resistance is proportional to the strain
  experienced by the sensor.
Strain gauge
• If a wire is held under tension, it gets
  slightly longer and its cross-sectional
  area is reduced. This changes its
  resistance (R) in proportion to the strain
  sensitivity (S) of the wire's resistance.
  When a strain is introduced, the strain
  sensitivity, which is also called the gage
  factor (GF), is given by:
              GF = (ΔR/R)/(ΔL/L)
Strain gauge
• The ideal strain gage would change
  resistance only due to the deformations
  of the surface to which the sensor is
  attached.
• However, in real
  applications, temperature, material
  properties, the adhesive that bonds the
  gage to the surface, and the stability of
  the metal all affect the detected
  resistance.
Strain gauge
• Because most materials do not have the
  same properties in all directions, a
  knowledge of the axial strain alone is
  insufficient for a complete analysis.
  Poisson, bending, and torsion strains
  also need to be measured. Each requires
  a different strain gage arrangement.
Strain gauge
• The most widely used characteristic
  that varies in proportion to strain is
  electrical resistance. Although
  capacitance and inductance-based
  strain gages have been
  constructed, these devices' sensitivity
  to vibration, their mounting
  requirements, and circuit complexity
  have limited their application.
Strain gauge
Physical Principle
   Ohm’s Law
       R = ρ L/A
       Combining Ohm’s Law with definition of strain ε:
               ∆R/R = (1+2v)ε+ ∆ρ/ρ= Gε
       First term: Under strain, wire changes dimension, and thus the resistance
        changes.       Dominant for metals.

        Second term: change in resistivity due to the change in the crystal lattice
         of the material under strain (piezoresistive effect). Dominant in
         semiconductors (but expensive).
    Foils/filaments inside the strain gauge are ~1/1000th inch
     diameter, made up of basic metal conductors.
Strain gauge
Load Cell Implementation
   Change in resistivity under strain is linear when ∆R/R is less than 1%
    → Small ∆V (mV level)
   Wheatstone Bridge Circuit is used with a strain gauge as one or more of its resistors:




                                                      Instrumentation Amplifier

   Applied force causes small change in resistance in strain gauge → change in output
    voltage across bridge circuit.
   Output voltage from bridge circuit is amplified using an instrumentation amplifier,
    usually to 0-5 or 0-10 V range.
   Circuitry housed in a mechanical device (the load cell casing itself).
   Algorithms determine actual force based on output voltage (usually outside load cell).
Application of Strain gauge
• Strain gages are used to measure
  displacement, force, load, pressure, torque or weight.
  Modern strain-gage transducers usually employ a grid of
  four strain elements electrically connected to form a
  Wheatstone bridge measuring circuit.
• The strain-gage sensor is one of the most widely used
  means of load, weight, and force detection.
• As the force is applied, the support column experiences
  elastic deformation and changes the electrical resistance
  of each strain gage. By the use of a Wheatstone
  bridge, the value of the load can be measured. Load
  cells are popular weighing elements for tanks and silos
  and have proven accurate in many other weighing
  applications.
Application of Strain gauge
• Strain gages may be bonded to cantilever
  springs to measure the force of bending.
• The strain gages mounted on the top of the
  beam experience tension, while the strain gages
  on the bottom experience compression. The
  transducers are wired in a Wheatstone circuit
  and are used to determine the amount of force
  applied to the beam.
Application of Strain gauge
• Strain-gage elements also are used widely in the
  design of industrial pressure transmitters. Using
  a bellows type pressure sensor in which the
  reference pressure is sealed inside the bellows
  on the right, while the other bellows is exposed
  to the process pressure.
• When there is a difference between the two
  pressures, the strain detector elements bonded
  to the cantilever beam measure the resulting
  compressive or tensile forces.
Application of Strain gauge
• A diaphragm-type pressure transducer is
  created when four strain gages are attached to a
  diaphragm.
• When the process pressure is applied to the
  diaphragm, the two central gage elements are
  subjected to tension, while the two gages at the
  edges are subjected to compression.
• The corresponding changes in resistance are a
  measure of the process pressure. When all of
  the strain gages are subjected to the same
  temperature, such as in this design, errors due
  to operating temperature variations are reduced.

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Electric transducer

  • 1. Electric transducer (Load cell) Prepared by: Uday A. Korat (B.E. 3rd year(EC),LDCE)
  • 2. Electric transducer • A transducer is a device that converts one form of energy to another. Energy types include (but are not limited to) electrical, mechanical, electromagnetic (including light), chemical, acoustic or thermal energy. • Electric transducer: A device which converts any kind of energy into electric signal whether it is analog or digital.
  • 3. Types of Electric transducer • Sound -> Electrical (microphones) • Force -> Electrical (Load Cells) • Kinetic -> Electrical (piezoelectric, generators) • Light -> Electrical (solar panels) • Thermal -> Electrical (thermocouple)
  • 4. Load cell • Load cells are integrated sensors that measure weights and output continuous electrical, pneumatic, or hydraulic analog signals. • A load cell is generally comprised of three parts: a mechanical system, a strain gauge, and an electronic amplification device
  • 5. • The measurement of a force is done by the use of these three parts in the order they are listed. It should be noted that load cells can be configured with multiple "strain gauges".
  • 6. Strain gauge • When external forces are applied to a stationary object, stress and strain are the result. • Stress is defined as
  • 7. Strain gauge • Strain is defined as the amount of deformation per unit length of an object when a load is applied. Strain (ε) = ΔL/L • Typical values for strain are less than 0.005 inch/inch and are often expressed in micro-strain units: 1 μstrain = 106 strain
  • 8. Strain gauge • Strain may be compressive or tensile and is typically measured by strain gages. • It was Lord Kelvin who first reported in 1856 that metallic conductors subjected to mechanical strain exhibit a change in their electrical resistance. • This phenomenon was first put to practical use in the 1930s.
  • 9. Strain gauge • Fundamentally, all strain gages are designed to convert mechanical motion into an electronic signal. • A change in capacitance, inductance, or resistance is proportional to the strain experienced by the sensor.
  • 10. Strain gauge • If a wire is held under tension, it gets slightly longer and its cross-sectional area is reduced. This changes its resistance (R) in proportion to the strain sensitivity (S) of the wire's resistance. When a strain is introduced, the strain sensitivity, which is also called the gage factor (GF), is given by: GF = (ΔR/R)/(ΔL/L)
  • 11. Strain gauge • The ideal strain gage would change resistance only due to the deformations of the surface to which the sensor is attached. • However, in real applications, temperature, material properties, the adhesive that bonds the gage to the surface, and the stability of the metal all affect the detected resistance.
  • 12. Strain gauge • Because most materials do not have the same properties in all directions, a knowledge of the axial strain alone is insufficient for a complete analysis. Poisson, bending, and torsion strains also need to be measured. Each requires a different strain gage arrangement.
  • 13. Strain gauge • The most widely used characteristic that varies in proportion to strain is electrical resistance. Although capacitance and inductance-based strain gages have been constructed, these devices' sensitivity to vibration, their mounting requirements, and circuit complexity have limited their application.
  • 15. Physical Principle  Ohm’s Law  R = ρ L/A  Combining Ohm’s Law with definition of strain ε:  ∆R/R = (1+2v)ε+ ∆ρ/ρ= Gε  First term: Under strain, wire changes dimension, and thus the resistance changes. Dominant for metals.  Second term: change in resistivity due to the change in the crystal lattice of the material under strain (piezoresistive effect). Dominant in semiconductors (but expensive).  Foils/filaments inside the strain gauge are ~1/1000th inch diameter, made up of basic metal conductors.
  • 17. Load Cell Implementation  Change in resistivity under strain is linear when ∆R/R is less than 1% → Small ∆V (mV level)  Wheatstone Bridge Circuit is used with a strain gauge as one or more of its resistors: Instrumentation Amplifier  Applied force causes small change in resistance in strain gauge → change in output voltage across bridge circuit.  Output voltage from bridge circuit is amplified using an instrumentation amplifier, usually to 0-5 or 0-10 V range.  Circuitry housed in a mechanical device (the load cell casing itself).  Algorithms determine actual force based on output voltage (usually outside load cell).
  • 18. Application of Strain gauge • Strain gages are used to measure displacement, force, load, pressure, torque or weight. Modern strain-gage transducers usually employ a grid of four strain elements electrically connected to form a Wheatstone bridge measuring circuit. • The strain-gage sensor is one of the most widely used means of load, weight, and force detection. • As the force is applied, the support column experiences elastic deformation and changes the electrical resistance of each strain gage. By the use of a Wheatstone bridge, the value of the load can be measured. Load cells are popular weighing elements for tanks and silos and have proven accurate in many other weighing applications.
  • 19. Application of Strain gauge • Strain gages may be bonded to cantilever springs to measure the force of bending. • The strain gages mounted on the top of the beam experience tension, while the strain gages on the bottom experience compression. The transducers are wired in a Wheatstone circuit and are used to determine the amount of force applied to the beam.
  • 20. Application of Strain gauge • Strain-gage elements also are used widely in the design of industrial pressure transmitters. Using a bellows type pressure sensor in which the reference pressure is sealed inside the bellows on the right, while the other bellows is exposed to the process pressure. • When there is a difference between the two pressures, the strain detector elements bonded to the cantilever beam measure the resulting compressive or tensile forces.
  • 21. Application of Strain gauge • A diaphragm-type pressure transducer is created when four strain gages are attached to a diaphragm. • When the process pressure is applied to the diaphragm, the two central gage elements are subjected to tension, while the two gages at the edges are subjected to compression. • The corresponding changes in resistance are a measure of the process pressure. When all of the strain gages are subjected to the same temperature, such as in this design, errors due to operating temperature variations are reduced.

Notas do Editor

  1. First, a force is applied to the mechanical system, which transfers the force to the strain gauge, which is basically an elastic foil connected to a wheatstone bridge configuration. This wheatstone bridge configuration is the electronic device that the strain gauge uses to convert a certain amount of strain into electrical output. Essentially, the mechanical system and strain gauge are used to convert a force into an electrical output.
  2. This electrical output is generally very small, so it is amplified using a form of electric amplification, for which an integrated circuit or transistor may possibly be used. The electrical output is measured and the plugged into a computer algorithm. The algorithm uses the amount of electricity to tell a user how much force was applied to the load cell.