Displacement and Motion Flashcards

1
Q

Linear variable resistors

A

e.g. rheostat.
Changing length of resistor used changes
resistance, can attach moving object to slider.
§ Use as a voltage divider
§ Has high sensitivity, moderate precision
and large range (up to 100mm)

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2
Q

o Strain gauge

G= change in R/ R
over change in L/ L

A

Made using constantan conductors laminated between polymide film
and can be uniaxial, biaxial or triaxial. Resistivity increases as tensilenstress is applied to a wire.
§ Often used in a Wheatstone bridge with an instrumentation amplifier
§ Foil/silicon strain gauge has low/high sensitivity, moderate precision and small range
§ Be able to show how to use strain gauges in Wheatstone Bridge on cantilever beam

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3
Q

o Liquid metal strain gauge

A

Elastic resistors are constructed by filling a
compliant elastic tube with a conductive
fluid (e.g. aqueous electrolytes)
§ Gauge produces a force which depends upon
the elastic properties and geometry of the
elastic tubing. Must be kept in tension to
avoid buckling the tube.
§ Are inexpensive and simple to construct.

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4
Q

o Piezo-electric strain sensors

A

§ Charges displaced in response to mechanical stress.
§ Mostly used for measuring alternating strain in vibrating structures.
§ Inherently very stiff and are typically used as force sensors and pressure sensors.

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5
Q

Eddy-Current Sensors

A

§ Uses Lenz’s law
§ A high frequency current is
generated in a coil.
§ The magnetic field created by the coil passes through a
conducting target attached to
the moving surface.
§ The changing magnetic field generates eddy currents in the target.
• Eddy currents = a localized electric current induced in a
conductor by a varying magnetic field
§ The eddy currents alter the impedance of the coil.
§ The change in impedance can be measured as a change in the
amplitude and/or phase of the current through the coil
§ Are simple, low-cost and light weight, rugged, unaffected by dirt,
moisture, high bandwidth
§ Need to be linearised

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6
Q

o LVDT

A

Consists of a primary coil and
two secondary coils
symmetrically spaced from the
primary. The ferromagnetic
core can move axially within
the coils. The primary coil is
excited by an AC which
produces a magnetic field that
induces voltages in the two
secondary coils.
§ The secondary coils are connected in series opposition so that, when
the moveable ferromagnetic core displacement is in the middle, the
voltage generated in one secondary coil cancels the other.
§ When the ferromagnetic coil is displaced, the voltages induced in the
secondary cores are no longer equal, resulting in a nonzero output
voltage

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7
Q

o LVDT§ Properties:

A

• Made for a wide variety of length scales
• Relatively insensitive to temperature and aging
• Very sensitive
• No contact between the moving part of the sensor and the
coils
• Maximum frequency response is limited to well below the
frequency of the excitation voltage
• The moving core can add significant inertia to the item under
test

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8
Q

o Capacitive Modes

A
• Variable Spacing:
Capacitance decreases
in inverse proportion to
electrode spacing, while
impedance increases
linearly with electrode
spacing
• Variable area: Capacitance decreases linearly with change in
area, while impedance decreases in inverse proportion to the
change in area
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9
Q

o Capacitive Properties

A
  • Highest displacement resolution (~0.01 nm)
  • High linearity
  • High stability
  • Limited range (~100 �m to 1mm)
  • Moderate bandwidth
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10
Q

Hall-Effect:

A
• Charges flowing (in a current I
with velocity v) through a
conductor that is placed in a
magnetic field will experience
a Lorentz Force, given by:
• F = qV × B
• The force on the charges moves them in a direction
orthogonal to the magnetic field, creating a voltage, V.
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11
Q

o Hall-Effect Sensor

A

Using Hall-Effect to transduce a magnetic field into a voltage:
Mount a magnet near a Hall Effect sensor, can create a
displacement transducer (the movement of the magnet will
determine the force experienced by the charges and therefore
determine the voltage induced).
§ Relatively poor temperature stability, are inexpensive, good for
displacements < 25mm, non-linear

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12
Q

§ Michelson Interferometer

A
• Uses interference of
monochromatic light to
measure displacement
• As the moving mirror
moves toward or away
from the beamsplitter, the
interference pattern cycles
from constructive to
destructive every �/2
• The direction of movement
can be obtained by using
two interferometers in a quadrature configuration
• Ideal for measuring large displacements with very high
accuracy and high
speed
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13
Q

Heterodyne Interferometer

A
Light beam consists of
two frequencies of
similar wavelength
light to produce beats
at the optical receiver.
• Change in beat
frequency is directly
proportional to the
velocity of the moving
target. The measured velocity can then be integrated to
provide a measured change of position.
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14
Q

Optical Cross Correlation

A

• Motion detect between two images by performing crosscorrelation between subimages of each image

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15
Q

§ Optical Stereography

A

• Uses the information obtained from multiple cameras to
determine the position of points in space.
• Using Euclidean geometry, the position of a point can be
calculated from the location of the image of the point in the
cameras and a knowledge of the camera positions
• Accuracy of position estimation is dependent on the
resolution of the cameras, geometric distortion of the imaging
devices, knowledge of camera positions
• For dynamic imaging there is often a trade off between
spatial, temporal and image resolutions because of the rate
at which information can be moved from the camera to
memory

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16
Q
  • Accelerometers
A

o A sensor for measuring accelerations (!!)

o Usually constructed using MEMS techniques

17
Q

Gyroscope

A

o Measure rate of rotation of an object

18
Q
  • Electronic Compass
A

o Can be used to measure the orientation of device with respect to Earth’s
magnetic field
o Constructed of orthogonal magnetoresistive sensors arranged in a
Wheatstone bridge configuration
o Magnetoresistive sensors are thin-film resistors that exhibit a change in
resistance when exposed to an external magnetic field