Displacement and Motion Measurement

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Presentation transcript:

Displacement and Motion Measurement In the next two lectures we will discuss how to measure various types of displacement and motion These include: Linear Displacement Angular Displacement Linear Velocity Angular Velocity Acceleration Force

What is Motion? Motion or velocity can be defined in terms of the change in position of an object with respect to time All measurands of motion are some form of derivative of displacement with respect to time

Linear Displacement Is defined as specified distance in a specified direction It is measured in length units such as metres, kilometres etc. Symbol is s

Measuring Linear Displacement Very small displacements: Strain Gauges Capacitive Sensors Inductive Sensors (LVDT) Medium displacements Slide Wire / Film Wire wound potentiometer Large Displacements (above range of most ‘pure’ linear transducers) Convert linear to angular motion and measure the angular motion with an angular displacement transducer Measure velocity and integrate signal to obtain displacement

Linear Displacement - Resistive Methods Resistance is defined by the following equation Therefore if the length, thickness or resistivity of an object changes with respect to displacement we can use the resistance as a way to measure it

Linear Displacement - Resistive Methods (Slide Wire/Film) This is the simplest way of measuring displacement between a moving and a stationary object A piece of wire or film is connected to a stationary object A slide, which makes contact with the wire, is attached to the moving object This acts as a very basic potentiometer

Linear Displacement - Resistive Methods (Slide Wire/Film)

Pros and Cons – Slide Wire Range ± 1 – 300mm Advantages Simple Good Resolution Low Cost Disadvantages Wire does not have high resistance, film is better (±200 to 500Ω/cm) Wear Frictional Loading Inertial Loading

Linear Displacement - Resistive Methods (Wire Wound Potentiometer) Wire Wound potentiometers use the same principle as slide wire sensors except that they use a coil of insulated resistance The slider runs on one surface of the coil that is not insulated Taken from Novotechnik

Linear Displacement - Resistive Methods (Potentiometer)

Pros and Cons – Potentiometers Resolution ± 1mm – 4m Advantages Simple Robust Disadvantages Resolution dependant on wire diameter Continuous use over portion of the wire will cause wear Frictional Loading Inertial Loading

Linear Displacement - Resistive Methods (Strain Gauges) Attach the strain gauge to the object When the object is in tension or compressed it will result in a change in the resistance of the strain gauge This is used to measure the change in length of the object

Pros and Cons – Strain Gauges Advantages: Relatively easy to understand and attach Cheap Disadvantages Need temperature compensation

Linear Displacement - Capacitive Methods As we have seen in a previous lecture capacitance is defined as Therefore we could use the change in Plate Area Permittivity of the dielectric Distance between the plates as a way to measure displacement

Linear Displacement - Capacitive Methods (Variable Area) If we have an two electrodes and one moves relative to the other in a linear direction we will get an effective change in the area of the plates This results in a change in the capacitance which can be related to displacement

Linear Displacement - Capacitive Methods (Distance Between the Plates) If we have to electrodes, one fixed and the other movable we can arrange it that the distance between the plates changes for a change in displacement

Linear Displacement - Capacitive Methods (Distance Between the Plates) This type of capacitive arrangement consists of two fixed outer plates and one central moveable plate The central plate can move towards either of the plates which essentially changes the capacitance between the moveable plate and the fixed plates If the moveable plate is in the centre of the capacitor, voltages V1 and V2 will be equal

Linear Displacement - Capacitive Methods (Permittivity) The dielectric moves relative to the plates and this causes a change in the relative permittivity of the dielectric

Linear Displacement - Inductive Methods Inductive methods use very similar principles to resistive and capacitive methods The inductance of a coil is given by the following equation Where N is the number of turns in the coil, µ is the effective permeability of the medium in and around the coil, A is the cross sectional area and l is the length of the coil in m As with the other examples if we change any one of these parameters we get a change in the inductance

Linear Displacement - Inductive Methods (Linear Variable Differential Transformers LVDTs) LVDTs are accurate transducers which are often used in industrial and scientific applications to measure very small displacements

Linear Displacement - Inductive Methods (Linear Variable Differential Transformers LVDTs) An LVDT consists of a central primary coil wound over the whole length of the transducer and two outer secondary coils A magnetic core is able to move freely through the coil Taken from www.allaboutcircuits.com

Linear Displacement - Inductive Methods (Linear Variable Differential Transformers LVDTs) The primary windings are energized with a constant amplitude AC signal (1 – 10kHz) This produces an alternating magnetic field which induces a signal into the secondary windings The strength of the signal is dependant on the position of the core in the coils When the core is placed in the centre of the coil the output will be zero Moving the coil in either direction causes the signal to increase The output signal is proportional to the displacement

Linear Displacement - Inductive Methods (Linear Variable Differential Transformers LVDTs)

Pros and Cons - LVDTs Range: ±2.5nm - ±10cm Advantages: Disadvantages: Good resolution Disadvantages: Needs shielding to prevent interference from magnetic sources

Linear Displacement – Digital Methods It is also possible to measure displacement using digital methods As a binary system only uses 0’s and 1’s we can represent this using transparent and opaque areas on a glass scale or conducting and non conducting areas on a metal scale Each position will produce a unique code which represents a specific displacement