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FORCE

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Title: FORCE


1
MECHANICAL MEASUREMENTS
Prof. Dr. Ing. Andrei Szuder Tel.
40.2.1.4112604 Fax. 40.2.1.4112687 www.labsmn.pub.
ro szuder_at_labsmn.pub.ro
2
FORCE TORQUE MEASUREMENT
3
Force vs. Mass measurements
  • Balance systems compare weight of the known
    etalon with the force applied to the measuring
    arm

F
Fe
  • If the measured force, F is the weight of a
    stationary object, then we balance the mass of
    the object with the mass of the etalon.

4
Force MeasurementBy An ElasticElement
  • Elastic elements are often employed for force
    measurements via stress/strain Hookes law

Where K is the deflection constant and y is the
deflection at some characteristic point. Table
13.1 in the textbook lists some characteristic
cases
5
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6
Important note Do not confuse the deflection
constant K with the Bridge Constant, also
labeled by K!
7
Torque Measurements
  • Most often, torque sensors are used in measuring
    the power of rotary machines, hence their other
    name, dynamometers. In this use, we measure
    dissipated energy by applying brake load to the
    shaft of a rotary engine, and measuring the
    angular velocity and torque.

where T is torque, F is force at displacement R
from the axis of rotation and ? is an angular
velocity (rad/s)
8
Dynamometer types
  • The main challenges in dynamomemeter design and
    use are controlled energy dissipation and signal
    transmission from the rotary member to the
    stationary equipment (using some kind of
    brushes). Today wireless transmission systems are
    often used.
  • Based on the medium which dissipates energy
    (heat), dynamometers are classified as mecanical,
    hydraulic, electrical and transmission.
  • Transmission dynamometers are passive elements
    inserted into the system - they do not dissipate
    energy.

9
Torque Measurement By Different Strain
Gauge Configurations
10
Dynamic response Second Order Systems
  • Given the spring stiffness k, the damping
    coefficient c and the mass m, the spring/mass
    system with the damping element will follow

c
k
y
m
Fapplied
11
2nd Ord. System Response To A Step Function
If the system is excitedby a step function
The general solution can be expressed as
where
is the undamped natural frequency (in radians)
is the damped natural frequency (in radians)
is the critical damping ratio,
is the critical damping coefficient,
is the static displacement as time goes to
infinity and
is the response phase lag
12
The displacement due to an impulse signal will
depend essentially on two parameters the
critical damping ratio, ?, and the undamped
natural frequency, ?n.
Underdamped systems will swing above the
equilibrium few times before they settle at the
final level, while overdamped systems approach
the steady state from one side only!
13
2nd Ord. System Response To A Harmonic Excitation
If the system is excitedby a harmonic function
it will pass through a transient stage and settle
into a stationary oscillation, with a certain
amplification ratio, yd /ys, and a phase lag, ? .
where
is the excitation cyclic frequency (rev/s) and
is the system undamped natural cyclic frequency.
14
Notice that undamped system excited at natural
frequency will reach infinite amplification
ratio, i.e. it will come into resonance with the
excitation force. In practice, we try to limit
the useful frequency range to 20-40 of the
natural frequency, and have the damping ratio of
around 70.
15
Torque measurement
  • Torque is measured by either sensing the actual
    shaft deflection caused by a twisting force, or
    by detecting the effects of this deflection.

16
Torque measurement
  • To measure torque, strain gage elements usually
    are mounted in pairs on the shaft, one gauge
    measuring the increase in length (in the
    direction in which the surface is under tension),
    the other measuring the decrease in length in the
    other direction

17
Torque measurement
18
Torque measurement
19
Torque measurement
20
Torque measurement
21
Torque measurement
22
Torque measurement
  • The excitation voltage for the strain gage is
    inductively coupled, and the strain gage output
    is converted to a modulated pulse frequency
  • Maximum speed of such an arrangement is 15,000
    pm.

23
Load cells
24
Load cells
  • Load cells became are the method of choice for
    industrial weighing applications

25
Load cells
  • Strain-gage load cells convert the load acting on
    them into electrical signals. The gauges
    themselves are bonded onto a beam or structural
    applied. In most cases, four strain gages are
    used to obtain maximum sensitivity and
    temperature compensation. Two of the gauges are
    usually in tension, and two in compression, and
    are wired with compensation adjustments
  • Piezoresistive Similar in operation to strain
    gages, piezoresistive sensors generate a high
    level output signal, making them ideal for simple
    weighing systems because they can be connected
    directly to a readout meter.

26
Load cells
  • Inductive and reluctance Both of these devices
    respond to the weight-proportional displacement
    of a ferromagnetic core. One changes the
    inductance of a solenoid coil due to the movement
    of its iron core the other changes the
    reluctance of a very small air gap.
  • Magnetostrictive The operation of this sensor is
    based on the change in permeability of
    ferromagnetic materials under applied stress. It
    is built from a stack of laminations forming a
    load-bearing column around a set of primary and
    secondary transformer windings. When a load is
    applied, the stresses cause distortions in the
    flux pattern, generating an output signal
    proportional to the applied load. This is a
    rugged sensor and continues to be used for force
    and weight measurement in rolling mills and strip
    mills.

27
Load cells
  • New Sensor Developments
  • Fiber optic load cells are gaining attention
    because of their immunity to electromagnetic and
    radio frequency interference (EMI/RFI),
    suitability for use at elevated temperatures, and
    intrinsically safe nature. Work continues on the
    development of optical load sensors.
  • Two techniques are showing promise
  • measuring the micro-bending loss effect of
    single-mode optical fiber
  • measuring forces using the Fiber Bragg Grating
    (FBG) effect.

28
Load cells
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