Properties and Effects
Because of the density and elasticity makeup of high density polyethylene,
sending and receiving ultrasonic pulses through the plastic is going
to be highly attenuated and this factor increases if you take into
account any fluid, such as water, flowing through the pipe. If we
were to compare attenuation or loss of acoustic energy from scattering
and absorption, it is absorbed about six times more than in carbon
steel. Reflection of the ultrasonic signal from the pipe backwall
is also of significance. Since the acoustic impedance constants of
water and the piping are closely related, the reflection coefficient
or the amount of ultrasound that returns from the pipe/water interface
(backwall), using a 6.4 mm (0.25 in.) diameter 2.25 MHz transducer,
is only 8 percent. The remaining 92 percent reflection coefficient
is absorbed into the water.
Velocity, impedance and attenuation
are all factors that will influence the ability to capture a thickness.
The signal strength will be greatly diminished, but with some adjustment
of the gain and proper selection of transducers, capturing a thickness
from a 51 mm (2 in.) wall is probable. Keep in mind that any internal
geometric changes from erosion rendering the pipe surfaces nonparallel
will create some diffraction and will contribute to an even lower
signal response. With this information in mind, we can now understand
some of the inherent problems that are encountered which should help
in the proper selection of transducers and instruments.
The difficulties discussed above
are going to be important when considering instrument and transducer
selection. You will need to experiment with transducer diameters and
frequencies to ensure that proper surface contact and a strong enough
pulse exist to punch through the ranges of pipe thickness. Using an
A-scan instrument with gating capabilities along with a digital readout
to three decimal points is really going to become important if you're
doing any material loss calculations. An A-scan thickness meter with
a digital readout and dual transducer will not provide a strong enough
pulse for any pipe wall thicker than 9.5 mm (0.4 in.). A conventional
off the shelf transducer of 2.25 or 5 MHz will be suitable for most
pipes up to 16 mm (0.63 in.) thick. As thickness increases, larger
diameter and lower frequency transducers will be needed.
Experience Speaks
I want to share a case of how we dealt with taking accurate thickness
readings on high density polyethylene pipe for a mining company transferring
tailings slurry. Originally, steel pipe was being used for the purpose
of transporting the slurry, but the abrasive and erosive effects caused
premature failure. The high density polyethylene pipe alone could
not withstand the pressures involved with moving the slurry and there
was no real data to support its holding up against this type of abrasive
action. Eventually a decision was made to use the high density polyethylene
pipe as a liner inside the steel pipe. To access the polyethylene
piping for thickness testing, 13 mm (0.5 in.) diameter holes were
cut out from the bottom center of the steel pipe and a threaded nut
was welded into place. A 13 mm (0.5 in.) diameter bolt was then inserted
that could be easily removed when taking thickness measurements. This
was now a numbered testing point for monitoring.
Baseline readings were to be taken
and subsequent followup readings gathered every quarter (three months)
to monitor any liner material loss from possible erosion. The sonic
velocity in the polyethylene pipe is about 2.5 times slower than in
steel, so for accurate thickness testing, a stepped calibration block
meeting the range of thickness of the same material was machined.
Machining high density polyethylene pipe accurately is much more difficult
than machining steel, but with the use of a micro thickness gage,
each step can be measured and recorded (Figure
1).
It was not until after the third
quarterly tests were done and the thickness data collected that noticeable
inaccuracies in the data were found. Some of the thickness numbers
increased while others decreased for no given reason and at random
data points. The calibrations were made throughout the day during
the entire process and curiously enough we were continually adjusting
parameters on the instrument. Unfortunately, our data were so out
of line that they became useless. Our baseline readings were in question
and useless for calculating erosion rates. It became evident that
we were uncertain as to which numbers gathered were even correct.
Temperature and Velocity
A closer look into the variables involved led us to discover that
small differences in the temperature of the polyethylene had a direct
relation to material velocity, much different from that of steel.
As the temperature of the pipe increased throughout the day, the velocities
became increasingly slower and the reverse happened as it decreased
in temperature. So depending on the season or even throughout the
day, temperature variations at each of the 200 testing points had
an effect on the thickness recorded. Even partly cloudy days which
produced shadowing effects were sensitive enough to influence the
outcome of data.
The data in
Table 1 show examples of the change in thickness when temperature
increases 5.5 °C (10 °F) and 16.7 °C (30 °F) without adjustment for
material velocity. A mere 5.5 °C (10 °F) change in temperature might
represent the difference in morning and afternoon while the 16.7 °C
(30 °F) change could easily represent the difference between winter
and summer. As noted below, temperature effects are more pronounced
as the thickness increases.
To compensate for the changes
in temperature and the changes it has on material velocity, a velocity
and temperature correlation table was developed (Table
2). To ensure that this data was accurate, a piece of high density
polyethylene pipe was sent to a manufacturer's NDT laboratory familiar
with our needs.
Calibration and Testing
Instrument calibration is first done on the high density polyethylene
pipe step wedge with a temperature gage (Figure
2) and the velocity on the instrument adjusted according to
Table 2. The zero offset of the transducer is also entered into
the instrument setup. A transducer is then placed on each step of
the block and checked against the measurements taken with the micro
thickness gage. This is a simple two step calibration check: take
the temperature and adjust the velocity accordingly. With the use
of a digital A-scan instrument, always record thickness data at the
same signal height as that of the calibration. If you calibrate at
80 percent screen height, record your thickness data at the same screen
height. Equally important is the placement of the gate height. It
should always remain at the same percent screen height level when
calibrating and recording thickness data and this information should
be included in the procedure.
Each test point will require that
a temperature measurement be taken with the use of a digital meter.
The temperature can then be compared to the correlating velocity in
Table 2 and the instrument
velocity can then be adjusted. If temperature readings are not taken,
the accuracy of the thickness data will fluctuate from winter to summer
as well as throughout the day. It is not uncommon to see the temperatures
change throughout the day since the pipe is black and absorbs the
sun's heat even through the steel. As noted on the chart, a change
of 16.7 °C (30 °F) on a 13 mm (0.5 in.) pipe wall could give you an
error of 0.6 mm (0.02 in.) if no velocity adjustments are made.
One variable that has not been
determined is the temperature difference of the outside diameter of
the pipe versus the inside diameter of the temperature. However, thickness
readings have been conducted for four consecutive years and found
to be very accurate by simply taking temperature readings on the pipe
exterior at each monitoring access point and disregarding any internal
wall temperature difference. A range of thicknesses from 6.4 to 57
mm (0.25 to 2.25 in.) has been taken with this method. The temperature
of the fluid through the pipe can change the internal wall of the
pipe lining as well. However, our experience shows that this has not
dramatically changed the accuracy of the readings over a time span
of four years.
Writing Procedures for Variables
Associated with the Test
Many of us believe that once the choices of the instrument and transducer
are made, calibration of the instrument for the most part really only
involves using a correct velocity and adjusting for the transducer
zero offset. Others believe this is incorrect. This is where a procedure
is necessary. This is a set of instructions for repeating and duplicating
all aspects of the testing from calibration to gathering information
and sharing this information from one technician to the next. Writing
a procedure may seem unnecessary for merely taking thickness readings,
but the whole point is that one technician may do it differently from
another and no one wants to memorize data setups, especially if the
test intervals are three months apart. When writing your procedure,
keep it in a language that everyone can understand short and simple,
but specific.
Knowing the many variables, such
as those listed below, and adjusting for them, will allow one to ensure
an accurate data set. One should recognize the importance of this
information and consider it part of the procedure. Here are some variables
to think about for a procedure:
-
selection of instrument
(should remain the same throughout the testing time span)
-
selection of transducers
(should remain the same throughout the testing time span)
-
range settings
-
gate settings (especially
recording the percent screen height)
-
percent screen
height of backwall before collecting data (60, 70 or 80 percent)
-
signal flank versus
point recording
-
temperature/velocity
adjustments
-
whether there are
fluids going through the pipe
-
pipe temperature
variation due to weather conditions
-
accuracy of temperature
at each test point
-
calibration of
the temperature instrument gage at the beginning of each testing
day
-
whether thickness
data is being taken in the same location each time.
Training of the Technician
and Full Understanding of Procedure
Always record from the flank of your signal if that is how you
calibrated it and make it a habit to record the lowest reading on
the instrument. Make sure to use a micro thickness gage for measuring
the step wedge. A machinist will not be able to get as accurate a
tolerance as a steel step wedge. Mark your step wedge with a permanent
marker no larger than the diameter of the transducer at the same location
as the thickness gage reading and be exact to eliminate any room for
error. This is where the temperature probe and transducer will be
placed each time for calibration. Take temperature readings at each
thickness monitoring location. Do not assume that the temperature
at the top of the pipe is the same as that along the side or bottom.
When you find an area that you want to monitor, scan the circumference
of the pipe after it has been in service for a while and use the lowest
reading as the monitoring location. Make your test points permanent.
Pick your point then draw a circle with a permanent marker, but do
not make it any larger than the diameter of the transducer. You
do not want to be scanning a 25 mm (1 in.) diameter area with a 6.4
mm (0.25 in.) transducer. Record your thickness reading only after
the mark is in place.
Typically, the erosion is going
to take place on the bottom in the center and in the case of the tailing
slurry it was within a range of 127 mm (5 in.) of the bottom center
for a 0.5 m (20 in.) pipe. Therefore, try to determine closely where
the testing points should be. Bends create erosion at different locations.
If the pipe takes a steep drop or if the velocity of flow increases
and has a turn, the worst areas may be on the side of the pipe.
A flanged pipe can create turbulence
and may increase erosion within a 0.3 m (12 in.) distance. It would
be best to take readings in several locations at least 0.3 m (12 in.)
before and after (for 0.5 m [20 in.] pipe) the flange; or better yet,
try to scan for the lowest area and mark it as one to monitor. We
found that the highest number of failures occurring from erosion were
within this flange area. Within 0.3 m (12 in.) of the flange, visual
testing revealed unusual wavy wear patterns 25 to 51 mm (1 to 2 in.)
apart, which is where it can become difficult to capture a thickness
if parallel surfaces do not exist.
* HARSCO Track
Technologies, 3434 E. 7800 S. #220, Salt Lake City, UT 84121; (801)
517-7431; e-mail <fishing@icw.com>.