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Guide
to Ultrasonic test system - LOPKUD-014
Software Revision 1.0 / 2002 |
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| Short
description of the working principle |
The device generates short sinusoidal burst, that is
amplified and drivers with high power sending
transducer. Receiver is able to receiver signal after
its propagation in investigated material and the OPKUD
card allows to see the received signal, precisely
measure time of flight etc. Each signal can be sorted,
compared with another signal etc. The software allows
to measure attenuation, changes in signal frequency
etc. Burst parameters, signal amplitude and much more
can be controlled from the software.
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Hardware |
LOPKUD-014 is
particularly well suited for measurements with high
power, low frequency (<100kHz) ultrasonic waves. It
can be used for testing materials with high
attenuation (scattering), such as stones, concrete,
wood etc. It can also be used for measurements with
air ultrasound (contact less transmission measurements).
The device has following elements:
- High power sender;
- High sensitivity selective receiver;
- Modified OPKUD card, containing TTL - burst
generator;
- Power supply (220V)
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| Technical
data: |
| I.
Card |
| A/D
converter: |
| -
Resolution: |
8bits |
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- Sampling frequency: |
4MHz |
| Analog
parameters: |
| -
Input channels: |
1
BNC |
| -
Output channel: |
1
BNC |
| -
Input amplifier gain: |
0dB,
6dB, 14dB, 20dB |
| -
Attenuator: |
-20dB |
| -
Input voltage: |
AC,
max. 10mVpp |
| -
Input impedance: |
200Ohm |
| Data
buffer: |
16K |
| Triggering: |
internal |
| II.
Sender |
| -
Frequency: |
200kHz |
| -
Output voltage |
max:
500Vpp |
| -
Burst length: |
2-128
cycles |
| -
Burst duration in % of time: |
<
2% |
| III.
Receiver |
| -
Selective |
200kHz |
| -
Amplification: |
40dB,50dB,60dB,70dB,80dB,90dB,100dB |
| -
Attenuator: |
20dB |
| Signals
on the external connectors: |
DB9
(male)
Ntrig - pulse generator control;
Kreg (out) - software controlled preamplifier gain
DB9 (female)
RS232
BNC (female)
Uin - measured input signal
BNC (male)
INPUT - input of receiver
OUTPUT - output of high voltage transmitting signal
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Software: |
In order to use
LOPKUD-system, following equipment is necessary:
Computer System: IBM PC
Display Adapter: SVGA Adapter working in mode 640x480
or higher (recommended 800x600)
Operations System: Windows 95, Windows 98, ME, XP and
Windows NT or 2000.
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Overview of Hotkey Selection: |
[F1] Open Load in a previously saved data file and
restore the capture settings as they were when the
data was saved
[F2] Save as This
option creates one file that contains both the current
settings and the current data. The setting saved are
the same in the Save Settings option.
[F3] Print This
option will create a hardcopy of the screen into IBM
Graphics mode compatible printers. The printout will
include everything currently on the screen.
[F4] About us…
Short information about OPTEL
[F5] Select port From
the settings window it is possible to change a board
address, and rs232 port.
[F6] Help a general
help screen is available that shows most hotkeys of
the program
[F7] RUN / STOP
enables / disables selected acquisition mode
F8] Zoom / Spectrum
choose between Zoom and Spectrum display in bottom
window (Zoom - zoom for timing display; Spectrum - A
set of functions which perform transformations between
the time domain and the frequency domain, and perform
analysis in the frequency domain. These functions are
based on the discrete implementation of the Fourier
Transform. Several rely on frequency domain
transformations to obtain the results indirectly).
[F9] RF Signal /
Detector Choose between RF Signal and Detector display
in upper and bottom window.
[F10] Exit Exit to
system
[F11] Show diagram
Show diagram of Ureg=f(N)
[F12] Transition [on/off]....
close and open of RS232 transmission from sender.
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On the scope screen: |
Memory three memories
for the measured signals
Grid ON/OFF toggle on/off the display of the division
grid
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Measuring - Cells: |
Markers from Signal
screen and Zoom / Spectrum screen.
Time of flight [us]: It is necessary to prepare the
signal, that will be compared (correlated) with the
actually measured signal. If the transducer sends a
short signal, it is no problem with choosing a proper
signal, but it is also possible to choose any other
signal. After the chosen signal is visible on the
Singal screen, and the markers positioned on the left
and right limit of the chosen signal, it is necessary
to switch the "Pattern". After it, the
bottom screen shows the chosen signal with the comment:
"Correlation Pattern". This step can be
repeated until the chosen signal is perfect. In the
second step the measurement should be started ("Measure").
Ureg[V].: sender signal amplitude
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Description of software for measurement of time of
flight. |
This software package
allows to measure time of flight.
For each measurement it is necessary to choose
reference signal and compare it with the signal,
coming from the measured medium (reflected or
transmitted through it). This allows to use this
software with almost any kind of samples, containments
etc. For people using this software it is necessary to
have some knowledge about such kind of measurements,
physics of ultrasounds etc
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I. Introduction to the work with the software |
First step
Reference signal should be prepared, the best way to
do it is to use pure (distilled) water. Using markers
in the upper window most important part of the signal
should be chosen. In the bottom window signal between
markers from the upper window can be seen - magnified.
See picture 1.

Picture 1.
Second
step.
Button
"Pattern" should be used. After pressing
this button, chosen signal appears in bottom screen in
white color together with information: "Correlation
pattern". It means this signal from this moment
will be "reference signal". See picture 2.

Picture 2.
From
this moment key called "Measure" should be
used - all subsequent operations will use signal
stored before (pattern) as reference for comparison
with actually measured signal. See picture 3. For time
of flight measurement the display will show 0 -
nothing changed.
Third step
In this moment we have to repeat operations described
in the first step. In upper window we choose - using
markers the most important part of signal we are
getting from measured medium. In the bottom window we
can see only signal between markers from the upper
window. See picture 4. Pay attention on marker
position (it is changed now). It means now we have
another signal (with time offset for example).

Picture 3.
In this
moment we have all information which is necessary for
calculation of time of flight (and another functions
too), and then the button "Measure" should
be used . On the bottom window we can see two earlier
prepared signals (white - reference signal; red -
measure signal) in this case we receive result
different from zero.
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II. The time of flight and sound velocity measurement
method. |
In most cases we can
assume, that the signal will change after propagation
- simple geometrical comparison of signals won't work
properly. This is the reason, why we are using
following algorithm for comparison of two signals with
different time of flight:
a) FFT with Hamming window is made.
b) In frequency domain, frequency with maximum
amplitude is chosen and using relatively sharp
windowing only this frequency and frequencies from its
neighborhood are taken.
c) Inverse FFT is done.
d) Center point of achieved signal is taken as time
mark, telling us the moment of "coming" of
this signal.
Time of flight can be measured from zero point (start
of pulse) or from the time of "coming" of
another signal, stored as pattern - as described above.
If the path length is known, it is possible to
calculate the sound velocity in the measured material,
using comparison with reference fluid - for example
water.
If the experimental setup have a containment with
measured fluid, where only a part of the sound
propagation path is in the measured fluid, we can
wrote following formula:
T=T1+T2
Where T1 is time of propagation outside of measured
fluid and T2 in this medium.
We can measure time of flight in the whole system (T)
filled with water (TW, that has velocity CW), or
measured fluid TX (velocity CX). If we know the path
length (L) in measured fluid, we can calculate the
velocity of sound in this medium:
T2w=L/CW
T1=TW-T2W
This (T1) can be obtained after measurement with water,
and this measurement must be done only from time to
time, since parameters of system doesn't change
quickly.
CX (sound velocity in measured medium) = L/(TX-T1)
The user of the software must know the path length
(L), and choose appropriate signals (not only direct
transmission must be chosen, but also multiple
reflections for example).
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LOPKUD 014.PDF
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