Page 387 - Mechatronics with Experiments
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October 9, 2014 8:1
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            JWST499-c06
                        JWST499-Cetinkunt
                                                                                        SENSORS  373  254mm×178mm
                             the ratio of change in the length to the total length in that direction,
                                                                  ΔL
                                                                 =                             (6.128)
                                                                  L
                             The change in the strain-gauge resistance is converted to a proportional voltage using a
                             Wheatstone brige,
                                                                   ΔR
                                                          V out  = K ⋅                         (6.129)
                                                                 1
                                                                    R
                                                                      ΔL
                                                             = K ⋅ G ⋅                         (6.130)
                                                                 1
                                                                       L
                                                                   ΔL
                                                             = K ⋅                             (6.131)
                                                                 2
                                                                    L
                                                             = K ⋅                             (6.132)
                                                                 2
                             Note that a strain gauge has a finite dimension. It is bounded to the surface of the part over
                             a finite area. Therefore, the measured strain is the average strain over the area occupied by
                             the strain gauge. The bonding of the strain gauge to the workpiece is very important for
                             two reasons: (i) it needs to provide a uniform mechanical linkage between the surface and
                             sensor in order to make the measurement correctly, (ii) the bonding material electrically
                             isolates the sensor and the part. The strain gauges themselves have a very high bandwidth.
                             It is possible to build strain gauge sensors that have almost 1 MHz bandwidth. Using silicon
                             crystal materials, strain gauge size can be minaturized while having a very large sensor
                             bandwidth.


                             6.7.2 Force and Torque Sensors
                             Force and torque sensors operate on the same principle. There are three main types of force
                             and torque sensors,
                                1. spring displacement based force/torque sensors,
                                2. strain-gauge based force/torque sensors,
                                3. piezoelectric based force sensors.
                                  Let us consider a weighing station as a force sensor application. If we have a calibrated
                             spring with a known spring coefficient, K spring , the load force (for torque measurement, we
                             would use an equivalent torsional spring) can be measured as displacement,

                                                            F = K spring  ⋅ x                  (6.133)
                             Using any of the position sensors, the displacement x can be converted to a proportional
                             voltage, and hence we obtain the force (or torque) measurement,
                                                            V   = K ⋅ x                        (6.134)
                                                             out   1
                                                                = K ⋅ F                        (6.135)
                                                                   2
                                  The strain-gauge based force and torque sensors measure the force (or torque) based
                             on the measured strain. Again, the sensor relies on an elastic sensing component. Typical
                             force/torque sensors are called load cells. A load cell has built in elastic mechanical
                             components on which strain gauges are mounted (Figure 6.44). As the load cell experiences
                             the force (or torque), it deforms a small amount which induces a strain on the sensing
                             element. The strain is measured by the strain gauge. As a result, since the force/torque to
                             strain relationship is linear by the design of the load cell, the measurement is proportional
                             to the force/torque.
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