ISonic 2009 - UPA Scope
The Sonotron ISonic 2009 UPA-Scope - Portable High Performance Ultrasonic Phased Array Flaw Detector & Recorder with Conventional UT & TOFD Channels
THE VERSATILITY OF ULTRASONICS
Phased Array Modality Conventional UT and TOFD Modalities
·
1, or 8, or 16 channels · 100% raw data capturing · Powerful off-line data analysis toolkit · Intuitive User Interface · Light rugged case · Sealed keyboard and mouse · Large 8.5” bright touch screen · Ethernet and 2 X USB Ports · Remote control - UT over IP · Built-in encoder port ISONIC 2009 UPA Scope uniquely combines phased array, single- and multi-channel conventional UT, and TOFD modalities providing 100% raw data recording and imaging. Along with portability, lightweight, and battery operation this makes it suitable for all kinds of every-day ultrasonic inspections Phased array modality is performed by powerful 64:64 phased array electronics with independently adjustable emitting and receiving aperture, each may consist of 1 through 64 elements. Groups of phased array probe elements composing emitting and receiving aperture may be fully or partially matching or totally separated allowing flexible managing of incidence angles, focal distances, types of radiated and received waves including directly reflected and diffracted mode converted signals Each channel is equipped with it's own A/D converter. Parallel firing, A/D conversion, and ”on-the-fly” digital phasing are provided for every possible composition and size of the emitting and receiving aperture. Thus implementation of each focal law is completed within single pulsing/receiving cycle providing maximal possible inspection speed Depending on configuration ISONIC 2009 UPA Scope carries 1, 8, or 16 additional independent channels for conventional UT and TOFD inspection and recording capable for both single and dual modes of pulsing/receiving High ultrasonic performance is achieved through firing phased array, TOFD, and conventional probes with bipolar square wave initial pulse with wide-range-tunable duration and amplitude. Maximal amplitude of bipolar square wave initial pulse is 300 V pp for phased array and 400 V pp for conventional channels. High stability of the amplitude and shape of the initial pulse, boosting of all it's leading and falling edges, and electronic damping are provided by the special circuit significantly improving signal to noise ratio and resolution. Thus analogue gain for each modality is controllable over 0…100 dB range Large 800X600 pixels 8.5” bright screen provides fine resolution for all types of inspection data presentation ISONIC 2009 UPA Scope is fully compliant with the following codes
·
ASME Code Case 2541 - Use of Manual Phased Array Ultrasonic Examination Section V
General
Technical Data
Phased Array Pulser Receiver
Phased array pulser receiver is controlled through intuitive operating surface comprising user interface of conventional ultrasonic flaw detector and ray-tracing graphics. Type of wave generated in the material is controlled through key in of corresponding ultrasonic velocity. Trace of ultrasonic beam is truly imaged upon entering thickness, outside diameter, and other suitable geometry data characterizing object under test - this extremely simplifies creating of focal laws and calibration of the instrument as well
Typical Phased Array Pulser Receiver screen of ISONIC 2009 UPA Scope B-Scan / S-Scan Cross-sectional insonification and imaging of the material may be provided electronically with use of linear array probes through:
·
Linear scanning with ultrasonic beam at predetermined incidence angle through reallocating of fixed size emitting/receiving aperture within entire array and composing of B-Scan image
Typical B-Scan indication of ISONIC 2009 UPA Scope representing inspection of composites for laminations: 1- scanning surface; 2 - bottom surface; 3 - lamination; 4 - A-Scan corresponding to the position of cursor over image The effects of inequality of elements of linear array, varying sound path and loss in the delay line or wedge, dependency of energy of refracted wave and effective size of emitting/receiving aperture on incidence angle should be compensated to equalize the sensitivity over insonified cross-section. The unique feature of ISONIC 2009 UPA Scope is the ability of managing independently adjustable focal laws within the same frame-composing sequence of pulsing/receiving shots so every focal law may me executed with individually adjusted gain, time base, and other core settings providing:
·
Gain per Shot Correction for B-Scan
S-Scan produced by ISONIC 2009 UPA Scope for several equal reflectors in the material with use of wedged linear array probe: 1 - angle gain compensation (AGC) is inactive; 2 - AGC is active; 3 - typical AGC graph
Regular (4) and true-to-geometry (5) S-Scan produced by ISONIC 2009 UPA Scope for compact reflector located at 20 mm depth of 40 mm thick plate. On the regular S-Scan single compact reflector is indicated twice for half (6) and full (7) skip detection while on the true-to-geometry S-Scan single reflector is shown in the real position once for both ways of detection (8) Weld inspection is typical application benefited through use of True-to-Geometry imaging: upon defining geometry and entering dimensions operator is provided with intuitive ray tracing dialogue indicating actual coverage of the weld for the desired probe position and incidence angle steering range followed by live S-Scan with true-to-location defects indication. To ensure detection of variously oriented defects several S-Scan and B-Scan insonifications may be performed simultaneously with use of the same probe providing multi-group cross-sectional viewing and recording along whole inspected length True to Geometry Imaging
Testing of solid and hollow shafts, axles, rods, longitudinal seams, nozzles, etc are among other applications improved significantly thanks to the easy-to-interpret advantage of True-to-Geometry imaging vs regular S-Scan and B-Scan
True-to-Geometry S-Scan for single location and complete cross sectional image of the hollow shaft with defects obtained after full circumference scanning with linear array probe
True-to-Geometry S-Scan for longitudinal weld (1) and nozzle (2) Tandem B-Scan Tandem B-Scan is another unique feature of ISONIC 2009 UPA Scope being most effective technique for the detection of vertically situated cracks in welds, plates, tube and vessel walls, and the like. It may be implemented with use of wedged 64-elements linear array probe. On entering material thickness and defining a grid dividing object's cross section into corresponding cells the instrument determines insonification strategy automatically by such a way that focal points of emitting and receiving aperture do match in the center of each cell in subsequent pulsing receiving cycles covering cross section completely. Individual gain per focal law adjustment is provided to equalize overall sensitivity for the variety of incidence angles, sound path lengths and losses in the wedge and material. For each focal law time base of the A-Scan is re-arranged automatically to provide appearance of possible echo from each cell at 50%-position. Recorded echo heights are represented on the Tandem B-Scan. Placing mouse cursor (marker) over desired cell reproduces corresponding A-Scan and ray trace indication
3D Data Presentation - Top (C-Scan), Side, and End Projection Views is performed through line scanning with linear array probe either encoded or time-based at rectangle to the elements count direction. It is applicable for all types of cross-sectional insonification C-Scan & 3D
For line scanning every cross sectional view is recorded along with complete sequence of raw data A-Scans it is composed of. C-Scan image is switcheable between distance (thickness or defects depth) and amplitude map
Powerful off-line data analysis toolkit includes playing back cross sectional views and A-Scans, gain manipulation in ±6dB range for all recorded A-Scans followed by corresponding image update, all-standards-compliant gate-based evaluation of echoes, geometry and amplitude filtering, image slicing and profiling, determining projection dimensions and area size of defects, 3D-viewing, etc
Crack Sizing Sizing of near surface cracks may be implemented with use of 64-elements linear array probe. Separated emitting and receiving aperture producing and receiving longitudinal wave have common focal point, which is manipulated over vertical line between bottom and near surface of the material. For each focal law time base of the A-Scan is re-arranged automatically to provide appearance of every possible tip diffraction echo at 50% horizontal position. Recorded signal heights are represented on the Tip Diffraction B-Scan. Placing mouse cursor (marker) over desired cell reproduces corresponding A-Scan and ray trace indication. Upon tip diffraction echo has been detected the crack depth and remaining material thickness are determined with high precision through triangulation
Tip Diffraction B-Scan for linear array probe placed above the material without (1) and with (2) a crack:3 - lateral wave (LW) signal mark; 4 - back wall (BW) echo mark; 5 - BW echo representation on the A-Scan; 6 - tip diffraction echo mark; 7 - tip diffraction echo representation on the A-Scan; 8 - precisely defined crack depth; 9 - precisely defined remaining material thickness Defects pattern analysis may be carried with use of well-known Delta Technique allowing distinguishing between low risk compact volumetric defects and cracks. Shear wave insonification of the evaluated discontinuity is performed with receiving of both direct shear wave and diffracted longitudinal wave echoes using the same linear array probe. Both echoes have been evaluated automatically providing digital readout of so called K LS value, based on which defect pattern is determined Defect Analysis
Implementation of Delta Technique is extremely simplified as only one linear array probe placed into position of receiving maximized echo from evaluated discontinuity is used instead of pair of conventional shear wave and longitudinal wave probes. Corresponding screen of ISONIC 2009 UPA Scope indicates 2 individually adjustable A-Scans comprising direct shear wave echo (1) with A S amplitude, diffracted longitudinal wave echo (2) with A L amplitude, and digital readout of K LS value (3) rating A S /A L For single conventional channel operation ISONIC 2009 UPA Scope provides fully featured A-Scan inspection as well as line scanning recording and imaging of the following types: thickness B-Scan; flaw detection B-Scan for angle beam and straight beam probes; CB-Scan for guided, surface, and shear wave probes inspections; TOFD. This fully covers scope of functions implemented by very well known ISONIC 2005 / ISONIC STAR / ISONIC 2020 portable ultrasonic flaw detector and recorder of Sonotron NDT ISONIC 2009 UPA Scope instruments equipped with 8 or 16 channels additionally provide multi-channel strip chart recording with forming all known types of strips such as B-Scan, PE, TOFD, Coupling. For certain applications such as, for example, brush probe scanning strip chart is convertible into C-Scan. This fully covers scope of functions implemented by very well known ISONIC 2008 portable multi-channel ultrasonic flaw detector and recorder of Sonotron NDT Comprehensive off-line analysis and data reporting toolkit for all kinds of data captured using conventional UT and TOFD modalities is built-in Conventional UT & TOFD Remote control of ISONIC 2009 UPA is implemented through Ethernet port. The instrument is fully compatible with new UT over IP technology from Sonotron NDT allowing full control of the instrument, imaging, recording, and storage inspection data in the remote control computer Remote Control - UT over IP
ADVANCED NDT LIMITED,
Products and Specifications Subject to Change Without Notice. E & O.E.
|