heal.abstract |
Nowadays, composite materials are widely used in a variety of applications in marine and
automotive industries, aerospace, aircrafts, buildings, and sport equipment. Low weight and high
strength are the most predominant features of such materials which makes them a favorable
option for even wider use is many structures. Composite shafts, mainly carbon fiber reinforced
polymer, are a characteristic case where such materials have started to be used and research for
their development is steadily increasing. Especially in the marine sector, composite driveshafts
can also offer corrosion resistance, low bearing loads, reduced magnetic signature and higher
fatigue resistance among other advantages.
For driveshafts torque monitoring during operation is an essential need for measuring the
power transmitted to the propeller or for performance evaluation and process monitoring and
control of combustion engines or electric motors. Another aspect is the strain measurement of
shafts, or in general of other composite cylindrical structures (e.g. pipes, tubes), for stress
analysis which is related to Structural Health Monitoring.
The main aim of this thesis, therefore, is an overview of the methods that are used for torque
and strain measurements on such structures. In the context of this thesis methods that are
commonly used in commercial applications or other that are still in a more preliminary -
laboratory level are presented. Based on the technique and/or the sensors that are used, a first
categorization was made. Strain Gauges (SG) are the most widely used system for strain
measurement and many commercially available torque transducers are based on this technique.
For the connection between the rotating shaft and the stationary part of the measurement system
contact connection with slip rings or non-contact connection with either inductive power supply
and/or signal transmission or with wireless RF telemetry can be made. On composite shafts due
to their orthotropic behavior, SG are more difficult to be used and more aspects are needed to be
taken into account. Fiber Optic Sensors (FOS) are also under development for both SHM and
torque measurement but still in a laboratory level. Fiber Optic Rotary Joints (FORJ) and other
systems which use special lenses (Graded-Index or C-lenses) can be used for non-contact signal
transmission although the problem ingress/egress point of such systems on rotating driveshaft is
still unsolved. Twist angle measurement is also widely used in commercial off-the-selves systems
as it offers simultaneously speed measurement and can be mounted on already existing shafting
systems without disassembly. Lastly, other systems which utilize Surface Acoustic Waves
(SAW), Digital Image Correlation (DIC) or other techniques that are under development were
also found.
A static torsional test on a CFRP shaft was conducted in the Laboratory of Testing and Materials
(LTM) of the School of Applied Mathematics and Physical Science of NTUA in Athens in order
to check the validity of the TorqueTrak 10k torque meter from Binsfeld which is based on the
wireless RF telemetry signal transmission technique. For that reason, analytical estimation of
equivalent mechanical properties of the shaft was made and a split-disk test in ring-shaped specimens for the experimental calculation of the Young’s modulus in the hoop direction.
Although many problems were encountered in both experimental procedures, some useful
conclusions about the applicability of this torque meter on composite shafts could be drawn after
processing the results.
Finally, FEM analysis in ANSYS simulation program was conducted. Deviation between the
numerical and experimental torsional stiffness was observed. This is probably attributed to the
overestimation of material mechanical properties considered for the modelling of the shaft
(mainly E1) and some deviations in the geometry (thickness, exact orientation of layers). Lastly,
since the maximum torque achieved during the torsional test was much lower than the critical
buckling torque of the shaft obtained from FEM and analytical solutions, no safe estimation of
the torsional buckling modeshape could be made. |
el |