Title: FORCE
1MECHANICAL 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
2FORCE TORQUE MEASUREMENT
3Force 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.
4Force 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(No Transcript)
6Important note Do not confuse the deflection
constant K with the Bridge Constant, also
labeled by K!
7Torque 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)
8Dynamometer 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.
9Torque Measurement By Different Strain
Gauge Configurations
10Dynamic 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
112nd 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
12The 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!
132nd 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.
14Notice 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.
15Torque measurement
- Torque is measured by either sensing the actual
shaft deflection caused by a twisting force, or
by detecting the effects of this deflection.
16Torque 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
17Torque measurement
18Torque measurement
19Torque measurement
20Torque measurement
21Torque measurement
22Torque 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.
23Load cells
24Load cells
- Load cells became are the method of choice for
industrial weighing applications
25Load 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.
26Load 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.
27Load 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.
28Load cells