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CHAPTER 3
MATERIALS AND EXPERIMENTAL PROCEDURE
3.1 INTRODUCTION
Material selection is an important aspect of design and
manufacturing. Often the success of the manufacturing is critically dependent
on a material or materials performing as desired. The following may be
considered for selection of materials.
• Material characterization data base
• Flight/Ship/Automobile history
• Cost, availability, lead time.
The reinforcement material chosen is glass fiber. Fiber glass also
called glass fiber reinforced plastic or GFRP is a fiber reinforced polymer
made of a plastic matrix reinforced by fine fibers of glass. Fiberglass is a light
weight, extremely strong and robust material. Although strength properties
are somewhat lower than carbon fiber and it is less stiff, the material is
typically far less brittle, and the raw materials are much less expensive. Its
bulk strength and weight properties are also very favorable when compared to
metals and it can be easily formed using molding processes.
The materials used for preparation of laminates are procured and the
different type of specimens is prepared as per ASTM standard. ASTM D3039
standard is used for tensile test of composite laminates. Single lap joint tensile
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test specimen has been prepared according to ASTM D5868-01.Double lap
joint tensile test specimen has been prepared according to ASTM D 3528–96.
Laminated specimens have been prepared according to ASTM D5628-10 and
laminated lap joint specimen according to ASTM D7136.The ASTM E610-82
is the definition for Acoustic Emission, ASTM E976 STANDARD (1994
(AE)) is used for Pencil Lead Break Test.
3.2 MATERIAL PROPERTIES
The laminates were made from fiberglass roving (E-glass), LY 556/
Hardener HY 951 system for laminates with different orientation. The
properties are
Pot life : 30-60 minutes at 2000c
Curing time : 14-24 hours at 200 c
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The hardener HY 951 is thoroughly mixed with resin. If a large
quantity of a mixture is to be prepared and must be cooled, as otherwise
strong exothermic heat is developed and the mixture will gel in a short time.
3.3 METHODS OF LAMINATE PREPARATION
3.3.1 Hand Lay-Up Method
The simplest manufacturing technique adopted is laying down
unidirectional glass roving over a polished mould surface previously treated
with a releasing agent: after this, a liquid thermosetting resin is worked into
the reinforcement by hand with a brush or roller. The process is repeated a
number of times equal to the number of layers required for the final
composite. Epoxy resins are most commonly used with glass fibers because of
their good strength properties. Resin and curing agents are pre-mixed and
normally designed to cross-link and harden at room temperature. The major
advantage of this manufacturing process is its great flexibility, since it suits
most common mould sizes and complex shapes. Although tooling is normally
expensive, it can be re-used for several runs and the actual cost of the raw
materials make this process economically feasible.
3.3.2 Vacuum Bagging Method
Also known as vacuum moulding, it requires a pump that will make
use of atmospheric pressure to consolidate the material while curing by
applying vacuum to the mould cavity. Usually the fibers are placed on a
single mould surface and covered by a flexible membrane, sealed around the
edges of the mould. The space between the mould and the membrane is then
evacuated with a pump and the vacuum retained until the resin has cured.
Figure 3.1 shows an example of vacuum bagging as given by Kornmann et al
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(2005) where several layers of glass fabric were placed intercalated with
epoxy resin. When the stack reaches the desired amount of layers, it is
covered with a peel ply, a perforated film and a breather fabric and then
introduced into a vacuum bag. An inlet and an outlet are placed on the
breather fabric and then the bag is sealed with sealant tape. After that, vacuum
is applied and for this particular case hydraulic pressure is also applied.
Vacuum bagging processes normally deliver a better volume fraction ratio
since any excess resin is drawn out of the composite. Also, the presence of
voids is reduced due to the extra pressure applied. One disadvantage of this
technique is the difficulty in maintaining a good vacuum over very large
moulds from 10m. Also, particularly with epoxy resins, thick sections take
time to fabricate due to the exothermic nature of the cross linking reaction.
The reaction generates heat, which needs to be released for the resin to
consolidate.
Figure 3.1 Vacuum bagging technique
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3.4 SPECIMEN PREPARATION FOR DEFECT
CHARACTERIZATION STUDIES IN LAMINATES
3.4.1 Preparation of Laminates from Unidirectional Glass Fibers
GFRP composite laminates with different orientations such as
0o, 90o, cross ply (0o/90o), angle ply (+45o/-45o) of size 300 x 300 mm2 are
fabricated using vacuum bagging technique as shown in Figures 3.2 (a), (b)
and (c). Ten layers of unidirectional glass roving along with LY556 epoxy
matrix are used for the purpose of fabrication of the laminates.
(a) (b) (c)
Figure 3.2 (a) Zero degree orientation laminate (b) Angle ply laminate
(c) Cross ply laminate
3.4.2 Preparation of Tensile specimens from Unidirectional Glass
Fibers
ASTM D3039 Standard tensile specimens was cut using water jet
cutting (Figure3.3) from the fabricated laminate of size 280x18x3mm3 as
shown in Figure 3.4 to avoid machining defects and to maintain good surface
finish.
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Figure3.3 Specimens preparation using water jet cutting machine
Figure 3.4 ASTM D3039 standard tensile specimen
For pure resin specimen, epoxy LY556 alone is used. Aluminum
tabs of size 60 x 18 x 3 mm3 are used to reduce the grip noise and prevent
damaging the extremities of the laminate with possible unexpected failures
external to the grip length as shown in Figure 3.5.
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Figure 3.5 Specimens of epoxy matrix composite materials for tensile
test as per ASTM D3039
3.5 SPECIMEN PREPARATION FOR DEFECT
CHARACTERIZATION STUDIES IN LAMINATED JOINTS
WITH DIFFERENT ORIENTATION
3.5.1 Cutting of Specimens from the Composite Laminates
Specimens are cut from each GFRP laminate having dimensions
102x25.4x3mm3 for laminated joints, as show in Figure 3.6.
Figure 3.6 Specimens cut from water jet cutting machine
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3.5.2 Surface Preparation and Curing
Considering bonded joints the surface preparation takes an
important role in perfect bonding, hand abrasion technique was used to
introduce roughness in the surface. The entire mould with glass fabric lay-ups
has been kept in 24 hours for curing. The curing has been done properly at a
room temperature, to prevent the reduction in strength of the bond
drastically. The major defects found in bonding of two materials are
disbonding, porosity and voids are mostly due to improper curing. To prevent
dislocation of specimen in bond region proper load is applied.
3.5.3 Preparation of Aluminum Tabs
Aluminum Tabs of dimensions 25x25x3 mm3 has been prepared to
prevent the grip noise. Initially the surfaces of Aluminum tabs and specimen
are prepared by using emery sheet for good bonding. The specimen is then
allowed to cure for 24 hours under room temperature after bonding.
3.5.4 Specimen Specification for Joints
3.5.4.1 Single lap joint
Tensile test specimen has been prepared according to ASTM
D5868-01 from the fabricated laminate show in Figure 3.7. The dimension of
tensile specimen according to ASTM D5868-01are as follows:
Length - 179 mm
Width - 25 mm
Thickness - 3 mm
Gauge length - 129 mm
Bond length - 25mm
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Figure 3.7 Tensile test specimen of ASTM D 5868-01
3.5.4.2 Double lap joint
Tensile test specimen has been prepared according to ASTM D
3528–96 from the fabricated laminate shown in Figure 3.8. The dimensions of
tensile specimen according to ASTM D 3528–96 are as follows:
Figure 3.8 Tensile test specimen of ASTM D 3528–96
3.6 FABRICATION OF TEST SPECIMENS FOR ADHESIVE,
BOLTED, HYBRID AND LAP JOINT WITH ATTACHMENTS
3.6.1 Materials Used
The laminates were made following correct procedure as shown
earlier from fiberglass roving of E-glass (Figure3.9), LY 556/ Hardener HY
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951 system. The density, thickness of the fiber glass roving is 1.3334 x 10 -3
g/mm3, 0.2 mm respectively.
Figure 3.9 Fiber glass mat
3.6.2 Laminate Preparation Process
The required mould is placed on the table and a thin layer of resin is
applied on the surface of the lower mould and the first layer of glass fabric is
placed on the mould, rollers are used to squeeze the excess resin. The resin is
applied over the first layer and the second layer is placed over the first one.
The procedure is repeated with alternating layers of glass fiber and resin
mixture until all required thickness. The vacuum bagging and cured at a
pressure of 1 bar for 2 hours as shown in Figure 3.10.The GFRP laminate
obtained from the vacuum bagging will be having dimensions of
600x600x3.5mm3.
Figure 3.10 GFRP laminate under vacuum bagging
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3.6.3 Specimen Preparation for Joint Strength Analysis
The specimens are prepared using single lap joint technique. These
specimens are subjected to tensile testing with Acoustic Emission sensors
positioned at -40mm to +40mm from the centre of the specimen. Four to six
specimens are tested in each type. The failure strength, Load, Displacement,
and Event Location Data of the four different specimens are compared and
discussed.
As per ASTM D5868-01 standard tensile specimens of size
102x25x3.5mm3are cut from the fabricated laminates using water-jet cutting
to avoid machining defects and to maintain good surface finish as shown in
Figure 3.11.
Figure 3.11 Specimens cut from water jet cutting machine
Aluminum tabs of size 25x 25 x 3.5 mm3 are used to reduce the grip
noise. The specimens are attached by bolt, adhesive and hybrid (bolt and
adhesive). Specimens are prepared and attached using aluminium sheet for
attachment with a thickness of 0.8mm, 1.2 mm And 2.0 mm with varying the
angle of 300 and 450 as shown in Figure.3.12
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(a) (b)
Figure 3.12 Tensile test specimen prepared as per ASTM D5868-01 for
thickness of 0.8mm,1.2mm,2.0mm with varying angle for
attachment at 300and 450 (a) top view (b) side view
3.7 SPECIMEN PREPARATION FOR IMPACT TEST
3.7.1 Preparation of Normal Specimen
Impact test specimen has been prepared according to ASTM D5628-
10 from the fabricated laminate as shown in Figure3.13. The dimensions of
impact specimen according to ASTM D5628-10 are as follows;
Length - 58mm
Width - 58mm
Thickness - 3.5mm
Specification of the glass fiber lamina used:
Weave style - plain
Thickness - 0.23+0.02mm
Area weight - 320gsm
Thermal stability - continuous use up to 500 o c
Glass content - 97.5%
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Figure 3.13 Normal specimen
3.7.2 Preparation of Adhesive Lap Joint Specimen
Impact test specimen has been prepared according to ASTM D7136
from the fabricated laminate and attached with adhesive as shown in
Figure 3.14. The dimension of impact specimen according to ASTM D7136 is
as follows;
Length - 150mm
Width - 100mm
Lap length - 50mm
Thickness - 3.5mm
Specification of the glass fiber lamina used:
Weave style - plain
Thickness - 0.23+0.02mm
Area weight - 320gsm
Thermal stability - continuous use up to 500 o c
Glass content - 97.5%
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Figure 3.14 Single lap joint specimens for impact loading
3.7.3 Impact Testing on Composite Laminates
Laminates were subjected to drop impact test using a CEAST
Fractovis Drop impact tower (Figure 3.15). The normal impact specimens
with dimensions of 58mm x 58mm were clamped by using pneumatic fixtures
shown in Figure.3.16 (a). Adhesively bonded specimens with dimension
150mm x 100mm x 3.5mm were tested by using a suitable fixture as shown in
Figure 3.16 (b).
Figure 3.15 Fractovis plus impact testing machine
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Figure 3.16 (a) Normal specimen in fixture (b) Adhesively bonded
specimen in fixture
3.8 SPECIMEN PREPARATION FOR RESIDUAL STRENGTH
PREDICTION AND COMPARISION OF FAILURE MODES
3.8.1 Damage by Drop-weight Impact
Laminated specimens are prepared as per ASTM standard. The
specimens fabricated are divided into four categories. One group of
specimens are as-received, while the remaining specimens are subjected to
drop impact at three different heights using a CEAST Fractovis Drop impact
tower (Figure 3.17). The diameter of the hemispherical indenter is 12.7 mm
with a clamping.
Figure 3.17 Laminate with impact damage
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3.8.2 Determination of Depth using Ultrasonic A-SCAN
To determine the extent of damage due to impact Omni Scan MX
type Ultrasonic scan facility is used as shown in Figure 3.18.
Figure 3.18 Ultrasonic omni scan
3.8.3 Dressed Laminate
The impacted region is grinded by decreasing length from the top
surface (descending) as shown in Figure 3.19, maintaining the length of
impact region more than 20 times its depth for good strength of the bonding
patches. The thickness was maintained using vernier calipers correctly to
avoid deviation in the failure load values.
Figure 3.19 Dressed Laminate
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3.8.4 Repair Mechanism
The impacted or damaged specimens are repaired by scarf, single
lap and double lap methods. The repair mechanism involves the process
different technics. Glass fiber mat of different sizes (7mm x 18mm, 13mm x
18mm, 20mm x 18mm) are cut to apply patch in the grinded region. The
prepared layers are patched on the damaged region of the specimen as the
ascending order for scarf repair, using epoxy LY 556 & hardener HY 951.
The patched surfaces are prepared for the overlap; according to overlap length
the layers are prepared from glass fiber mat for the size 40mm, 50mm, 60mm
and three layers of lap for each specimen. In single lap, the three layers are
overlapped on one side of the patched region as per the length. In double lap,
the three layers are overlapped on both sides. All the overlapped specimens
are cured in room temperature for 24 hours and aluminum tabs of size 60mm
x 3mm x 18mm are bonded on the surface of prepared specimens using
epoxy-Araldite.
3.8.4.1 Scarf repaired specimen
Single lap of repair is done by layers of fiber cloth with resin
mixture is applied over the damage removed region in a pattern that the length
of each subsequent layers with increasing pattern of width, so that the inclined
region reduce the peel stress while applying load (Figure 3.20). The above
process is called as patching process. The wet layup technique is used here.
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Figure 3.20 Scarf repaired model specimen
3.8.4.2 Single lap repaired specimen
Single lap repair is done by layers of fiber cloth with resin mixture
is applied over the damage removed region in a pattern that the length of the
each subsequent layers to reduce the peel stress while applying load (Figure
3.21). The wet layup technique is used here. After the patching technique, the
overlapping the glass fiber layers as the number of 3 layers are placed on the
patching specimen.
Figure 3.21 Single lap repaired model specimen
3.8.4.3 Double lap repaired specimen
The same patching procedure is followed for the double lap repaired
specimen. After finishing the patching, the same patching procedure will be
followed. The overlapping is to be done on both sides of the specimen (Figure
3.22). The repair efficiency is determined by the changing overlapping length.
The repair efficiency is evaluated by the manufacturing of five specimens on
every overlap length. Compare the results by the tensile test and find the best
repair technique.
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Figure 3.22 Double lap repaired model specimen
The cured specimens are tested by the tensile test with AE and the
damage mechanism and the strength are compared to find the best repair
technique.
3.9 TENSILE TESTING SET-UP IN UNIVERSAL TESTING
MACHINE (UTM)
3.9.1 Tensile Testing of Glass/epoxy Composite Determination with
A.E. Sensors
The specimens prepared from the laminates are tested using an
INSTRON 3367 universal testing machine along with acoustic emission
monitoring as shown in Figure 3.23.
Figure 3.23 Tensile testing of glass/epoxy composite has been
determined with A.E. sensors
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3.9.2 Tensile Strength under AE Monitoring
The Specimens are subjected to uni-axial tension in 30kN
INSTRON 3367 Universal Testing Machine (UTM) under
acoustic emission monitoring using an 8-channel Acoustic
Emission setup supplied by Physical Acoustics Corporation.
The Specimens are mounted on the UTM machine and
dimension of the specimens are entered in the software.
The crosshead speed was maintained at a rate of 0.15mm/min
AE signals are recorded for each specimen.
3.10 ACOUSTIC EMISSION MONITORING
3.10.1 Equipment used in AE Monitoring
The process of AE monitoring is made possible using an array of
instruments. Each component has a unique role to play and is essential to
ensure proper monitoring. A brief description of each component is detailed
in this section.
3.10.1.1 Sensors
They are the key instruments that detect the mechanical transient
elastic waves generated from within a structure and convert them into
electrical signals. Usually piezoelectric resonant sensors are used for AE
testing. Figure 3.24 shows a plethora of various kinds of sensors available in
today’s market.
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Figure 3.24 Different types of Sensors
3.10.1.2 Couplants and holders
Sensors are placed on the surface of the material to be tested using
various couplants. These are mainly used to assist easy and complete
conduction of acoustic waves generated from the source. Commonly used
couplants are oil, glue, high vacuum grease, etc. Along with the use of
couplants, most field tests require additional holders (e.g. mechanical or
magnetic) to keep the sensors in place.
3.10.1.3 Pre-amplifiers
The main purpose of the pre-amplifier shown in Figure 3.25 is to
provide gain to boost and effectively and reject noise from areas outside the
sensor operating range.
Figure 3.25 Pre-amplifier
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3.10.1.4 Data acquisition system
Modern AE systems use computers and appropriate software
providing a menu- driven parameter input and system control. All the signals
received at the sensor end are acquired and stored in the acquisition system.
The new generation systems also enable extensive post-processing
possibilities. Acquisition systems have also been well adapted for continuous
monitoring of structures using wireless technology and web-based remote
monitoring. Figure 3.26 represents the schematic representation of acoustic
emission testing set up.
Figure 3.26 Acoustic emission monitoring Process
3.10.2 A Generic AE System
A schematic representation of an acoustic emission system and its
detection procedure is represented in Figure 3.27. The process chain basically
consists of the following stages, which take place in a very short time, so that
all stages can be perceived as simultaneous for testing purposes.
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Figure 3.27 Schematic representation of acoustic emission (AE)
3.10.2.1 Acoustic emission setup
An 8 channel AE system supplied by Physical Acoustics
Corporation (PAC) is used for the study. The sampling rate and pre-
amplification are kept as 1 to 3 MSPS and 40 dB respectively. Preamplifiers
operating in the frequency band 10 kHz-2 MHz are used. AE activities were
sensed using wide band WD and NANO sensors, filtering out frequencies
exceeding 900 kHz and using a threshold of 45 dB to eliminate the back
ground noise. High vacuum silicon grease used as a couplant. The amplitude
distribution covers the range 0-99 dB (0 dB corresponds to 1µv at the
transducer output). After mounting two transducers on the sample at a mutual
distance of 100 mm between them, so that they were both at the same distance
from the centre of the specimen length, a pencil lead break procedure was
used to generate repeatable AE signals for the calibration of each sensor.
Velocity and attenuation studies are performed on the laminates. The Pre-
Trigger values and the Hit length values are estimated as 26 µsec and 4K
respectively.
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3.10.2.2 Pencil lead break test
Among the characteristics of the AE instrumentation system,
sensitivity needs to be considered first. Of all the parameters and components
contributing to the sensitivity, the piezoelectric sensor is the one most subject
to variation. This variation can be a result of damage or aging, or there can be
variations between nominally identical sensors (ASTM Standard E 1781). To
detect such variations, it is desirable to have a method for measuring the
response of a sensor to an acoustic wave. Specific reasons for checking
sensors include: (1) checking the stability of its response with time; (2)
checking the sensor for possible damage after accident or abuse. A
recommended method to check the sensitivity of the sensor is the response of
the system to pencil lead break test (ASTM E976 1994). In this test, a
repeatable acoustic wave can be generated by carefully breaking a pencil lead
against the test panel. When the lead breaks, there is a sudden release of stress
on the surface of the panel where the lead is touching. This stress release
generates an acoustic wave. The Hsu pencil source uses a mechanical pencil
and the Nielsen source can be used to aid in breaking the lead consistently.
The pencil lead break test was performed to obtain the actual AE source for
this research. The test scheme is shown in Figure 3.28 (ASTM E976
STANDARD (1994).
Figure 3.28 Hsu-Nielsen source (NDT.net 2007)
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3.10.2.3 Hsu –Nielsen source
Hsu-Nielson device (named after developer of the technique) is an
aid to simulate an acoustic emission event using the fracture of a brittle
graphite lead in a suitable fitting. This test consists in breaking a 0.5 mm
diameter
(2-H) pencil lead approximately 3 mm (+/- 0.5 mm) from its tip by pressing it
against the surface of the piece. This generates an intense acoustic signal,
quite similar to a natural AE source that the sensors detect as a strong burst.
The purpose of this test is twofold. First, it ensures that the transducers are in
good acoustic contact with the part being monitored. Generally, the lead
breaks should register amplitudes of at least 80 dB for a reference voltage of 1
mV and a total system gain of 80 dB. Second, it checks the accuracy of the
source location setup. This last purpose involves indirectly determining the
actual value of the acoustic wave speed for the object being monitored.
3.11 INPUT PARAMETERS TO AE WIN SOFTWARE
3.11.1 Wave Velocity
The wave velocity is calculated by Hsu Nielsen pencil lead break
procedure method as shown in Figure 3.29. The pencil tip is broken at a
known distance from the sensors and the corresponding time difference at
which the signal is captured by the two sensors is noted down. Then the wave
velocity is calculated from the following relation.
Distance between the sensors dWaveVelocity
Time interval at which signal is detected
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Figure 3.29 Wave velocity calculations
3.11.2 Wave Velocity Study
The Acoustically emitted sound waves travel with different velocity
in different types of materials. The wave velocity must be found to determine
the other Acoustic Emission parameters. So the velocity is calculated using
the following steps.
Initially the sensors are fixed at two locations in the specimen
(Figure 3.30).
High vacuum grease is applied on the sensor and then fixed
using tape.
The distances between the two sensors are measured.
Velocity study is done using Hsu-Nielson source (pencil lead
break).
The test is performed at various locations within the sensors.
Then the velocity is calculated using the formula.
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47 A.E. Sensor Position 80 47
Sensor 1
2
Figure 3.30 A.E. Sensor position
3.11.3 Hit Definition Time (HDT)
The function of Hit Definition Time is to enable the system to
determine the end of the hit, close out the measurement processes and store
the measured attributes of the signal. Proper setting of HDT ensures that the
AE signal from the structure is reported as one and only signal. The
recommended range for the composites is 100-200µs (SAMOS AE user
manual, Rev:2).
3.11.4 Hit Lockout Time (HLT)
The function of Hit Lockout Time is to inhibit the measurement of
reflections and late arriving parts of the AE signal. With proper settings of the
HLT, spurious measurements during the signal decay are avoided and data
acquisition speed can be increased.
3.11.5 Peak Definition Time (PDT)
The function of peak definition time is to enable determination of
the time of true peak of the AE waveform. A proper setting of the PDT
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ensures correct identification of the signal peak from rise time and peak
amplitude measurements. The recommended range for the composites is
20-50µs (SAMOS AE user manual, Rev:2). PDT is calculated using the
following relation.
Distance between the sensors PDTWave Velocity
3.11.6 Data Acquisition Process
Monitoring of AE signals generated from uni-axial Tensile
Test is done by an acquisition system.
The signals were detected using two Nano 30 piezoelectric
transducers, which are attached to the specimen surface using
high vacuum grease as a couplant and are fastened by tape.
The signals from the transducer passed through PAC 2/4/6
G/A pre-amplifier before reaching the main unit.
Wave velocity test is performed on the specimen and wave
velocity is calculated.
Next the sensors are connected to the 8-channel AE data
acquisition system.
UTM is switched ON and the tensile load is applied.
Various AE parameters such as Amplitude, Counts, Energy,
Rise, and Duration are recorded during the test.
The data are processed.
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3.11.7 Sample Rate
This is the rate at which the data acquisition board samples the
waveforms on a per second basis. A sample rate of 1 MSPS (Mega sample per
second) means that one waveform sample is taken every µsec.
3.11.8 Pre-Trigger
This value tells the software how long to record (in µsec) before the
trigger point (the point at which the threshold is exceeded). The user may
enter a value in the pre-trigger edit box. The minimum allowable pre-trigger
value is zero. The maximum allowable pre-trigger value is calculated by
dividing the hit length by the sample rate in MHz If, for example the hit
length was 1k(1k = 1024) and the sample rate was 4 MHz, then the maximum
allowable pre-trigger value would be 1024/4 = 256 µsec.
3.11.9 Hit Length
This determines the size of a waveform message. The available hit
length is in the range of 1k- 4k. At a 4 MSPS sampling rate, a hit length of 1k
will allow up to 256 µsec of data, a hit length of 2k will allow 512 µsec of
data (2*256) and so on.
The timing parameters in the hardware settings are calculated for
different materials and are listed in Table 3.1. The HDT is calculated from
trial and error method. Proper setting of the HDT ensures that each signal
from the structure is reported as one signal only.
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Table 3.1 Timing parameters for glass fibre
HDT(µs)
PDT(µs)
HLT(µs)
Wave Velocity m/s
Glass fiber/epoxy ( Unidirectional)
160 32 300 3078
Glass fiber/epoxy ( Bidirectional)
300 30 600 3020
The description of the sensors used in the experiments is listed in
Table 3.2.The calibration certificates for both Nano30 and Wide Band sensors
are shown in Figures 3.31(a) and 3.31(b) respectively.
Table 3.2 Description of sensors
Sensors Model
Sensors Dimensions DIA X HT
(mm)
Operating Temperature
( 0C )
CaseMaterials
Operating Frequency
Range (kHz)
Nano 30 PAC
8 X 8 -65 to 177 Stainless
steel125 - 750
WD (Wide Band)
18 X 17 -65 to 177 Stainless
steel100 - 1000
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3.12 SCANNING ELECTRON MICROSCOPE
3.12.1 Scanning Electron Microscope Test on Specimens
The S-3400N is a powerful, yet user-friendly SEM through newly
developed electron optical and automated functions. The famous Hitachi
image quality convinces at high and low beam energies, and optimized
detector technology provides maximum information from your sample.
Variable chamber pressure allows charge up-free observation of any sample
without special preparation techniques such as coatings shown in Figure 3.31
(a). All samples must also be of an appropriate size to fit in the specimen
chamber and are generally mounted rigidly on a specimen holder called a
specimen stub as shown in Figure 3.31(b).
(a) (b)
Figure 3.31 (a) Scanning Electron Microscope (b) Specimens in SEM
setup for testing
3.13 SUMMARY OF EXPERIMENTAL PROCEDURE
In the present chapter, materials used and the different methods for
manufacturing fiber reinforced composite plates were explained; the different
fabrication techniques were described along with the production of laminates.
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Preparation of the specimens as per ASTM standards for different loading
conditions is also discussed in this chapter. The tensile test equipment was
described; one 30 kN load cell Instron 3367 Universal testing machine was
used for all the tests. Drop impact test was conducted using Fractovis drop
impact tower. Scanning Electron Microscope S-3400N was used to identify
the damages in the tested specimens.
All the necessary equipment required to conduct AE investigation
have been described along with the terminology of the standard data
processing associated with AE. The sensors used in this research, their
technical specifications are also presented. The recording apparatus was
described thoroughly including the response from the system and how the
signal is modified while travelling from the material to the processing
software. A common way of calibrating an AE test in order to ensure some
repeatability is described in detail. There are also several other parameters
that need to be defined prior experimentation in order to make the best out of
the recording system and obtain sensible data. The procedure involved in the
selection of these AE hardware parameters for different materials are
presented in this chapter. All the input parameters for the experimentation
purpose are also presented in this chapter. More details about the geometries
selected after damage observation are given in the following chapter.