|
Guide to
Ultrasonic test system - USTS-011
Software Revision 1.0 / 2002
|
| |
| Hardware |
OPBOX-01/100 is particularly well suited
for ultrasonic measurements as well as other kinds of measurements which
employ mechanical scanning elements or multiplexed channels (the card is
capable of controlling such devices). Together with the pulser &
receiver unit and an ultrasonic probe it could be used as complete
ultrasonic testing device.
|

|
| Technical
data: |
| A/D
converter: |
| -
Resolution: |
8bits |
|
- Sampling frequency: |
2MHz |
| Analog
parameters: |
| -
Input channels: |
1
BNC |
| -
Output channel: |
1
BNC |
| -
Input amplifier gain: |
0dB,
6dB, 14dB, 20dB, 26dB, 34dB, 40dB |
| -
Attenuator: |
-20dB |
| -
Input preamplifier gain: |
20dB,
30dB, 40dB, 50dB, 60dB, 70dB, 80dB |
| -
pre attenuator: |
-20dB |
| -
Input voltage: |
AC,
max. 20mVpp |
| -
Input impedance: |
700Ohm |
| -
Output voltage: |
max:
1000V |
| Data
buffer: |
4K |
| Triggering: |
external
(TTL Signal) |
| Signals
on the external connectors: |
DB9
Uin - measured input signal;
Ntrig - pulse generator control;
Kreg (out) - software controlled preamplifier gain
BNC
Uin - measured input signal
Ext_trg - external trigger
|
|
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.
|
|
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.
|
|
On the scope screen: |
Memory three memories for the measured
signals
Grid ON/OFF toggle on/off the display of the division grid
|
|
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
|
|
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
|
|
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.
|
|
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).
|
|

USTS 011.PDF
|