where expertise comes together - since 1996 -

# The Largest Open Access Portal of Nondestructive Testing (NDT)

Conference Proceedings, Articles, News, Exhibition, Forum, Network and more

where expertise comes together
- since 1996 -

 Phoenix Inspection Systems LimitedDesign and manufacture ultrasonic Transducers, Scanners and Custom Solutions for NDT inspections. Innovators in NDT technology
 7826 views
Technical Discussions
Sunny
Sunny
00:26 Apr-02-2007

Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.

Thanks

Nigel Armstrong
Engineering, - Specialist services
United Kingdom, Joined Oct 2000, 1096

Nigel Armstrong

Engineering, - Specialist services
United Kingdom,
Joined Oct 2000
1096
04:50 Apr-03-2007
Sunny

Dead zone is demonstrated by use of a block of the same material provided with near surface side-drilled holes. The depth at which you first obtain a discernible response from one of the holes will identify the extent of the dead zone for the instrument/probe/material combination.

----------- Start Original Message -----------
: Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: Thanks
------------ End Original Message ------------

Sunny
Sunny
04:55 Apr-03-2007
----------- Start Original Message -----------
: Sunny
: Dead zone is demonstrated by use of a block of the same material provided with near surface side-drilled holes. The depth at which you first obtain a discernible response from one of the holes will identify the extent of the dead zone for the instrument/probe/material combination.
:
: : Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: : Thanks
------------ End Original Message ------------
Nigel,

What about using Flat Bottom Holes?

Roberto Falconio
Engineering, NDT/Metrology SUPERVISOR
El Salvador, Joined Feb 2000, 13

Roberto Falconio

Engineering, NDT/Metrology SUPERVISOR
Joined Feb 2000
13
04:58 Apr-04-2007
Hey guys,
Just my opinion, As far as I'm concern inmediately you plug the transducer you will appreciate that the initial pulse is some kind of wider making as a traingle shape (somtimes gets more irregular shapes), specially if your range is decreased. Under this conditions you can count the number of divisions between the flank of the initial pulse and where the "other traingle side" strikes the horizontal axis of the LCD. This is supposetly your dead zone area cause you may not display where an echo start in this zone (talking about the equipment). You may probably appreciate sometimes some echos peaks however you cannot discern where does its flanks are (always inside that zone). Nigel method might be more useful as you are testing with real discontinuities so you would expect to find a specific range. Just let me me know if its coincide with the area I'm talking about
Regards

----------- Start Original Message -----------
: : Sunny
: : Dead zone is demonstrated by use of a block of thesame material provided with near surface side-drilled holes. The depth at which you first obtain a discernible response from one of the holes will identify the extent of the dead zone for the instrument/probe/material combination.
: :
: : : Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: : : Thanks
: Nigel,
: What about using Flat Bottom Holes?
------------ End Original Message ------------

A. Anev
Teacher, NDT instructor
Vector NDT Ltd., Bulgaria, Joined Nov 1998, 2

A. Anev

Teacher, NDT instructor
Vector NDT Ltd.,
Bulgaria,
Joined Nov 1998
2
03:40 Apr-05-2007
The dead zone is measured for each system (transducer+cable+instrument) separately. And it would depend on the instrument gain and the required registration level (in terms of artificial flaw dimensions) for the given task. If you try to calculate it theoretically, the result may be very far away from the reality.
Is it possible that you need to calculate the near field length? excuse me for the question if this is not the case, but I saw many examples of these 2 terms misinterpreted.

----------- Start Original Message -----------
: Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: Thanks
------------ End Original Message ------------

Afshin
Consultant, NDT/QC/WELD INSPECTION
Iran, Joined Nov 2005, 20

Afshin

Consultant, NDT/QC/WELD INSPECTION
Iran,
Joined Nov 2005
20
01:49 Apr-11-2007
DEAR FRIEND,
FOR PRACTICAL DEAD ZONE CALCULATION,YOU CAN USE OF V1 BLOCK IN
AREA NEAR TO 50 mm DIA. PERSPEX .
---- Start Original Message -----------
: Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: Thanks
------------ End Original Message ------------

P V SASTRY
P V SASTRY
09:52 Apr-11-2007
Dear Sunny,

In pulse echo technique it varies with the gain setting too. So I advise not to bother too much about calculating the dead zone.

P V SASTRY

----------- Start Original Message -----------
: DEAR FRIEND,
: FOR PRACTICAL DEAD ZONE CALCULATION,YOU CAN USE OF V1 BLOCK IN
: AREA NEAR TO 50 mm DIA. PERSPEX .
: ---- Start Original Message -----------
: : Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: : Thanks
------------ End Original Message ------------

Debdutta Mallik
Consultant,
Malaysia, Joined Jun 2005, 37

Debdutta Mallik

Consultant,
Malaysia,
Joined Jun 2005
37
04:11 Apr-18-2007
Dear Friends,
Dead zone is a property of probe.So far I know it's not the property of instrument.Dead zone is the difference between electrical zero and real zero. Calculation may be very difficult unless having the step blocks.
Further informations are awaited related to the above.I'll be glad to know if there is any formulae for this.

Thanks,

Debdutta Mallik

TomNelligan
Engineering,
retired, USA, Joined Nov 1998, 390

TomNelligan

Engineering,
retired,
USA,
Joined Nov 1998
390
04:22 Apr-18-2007
Dead zone -- the interval following the excitation pulse in which potential exchoes are obscured by ringdown -- is a property of BOTH the probe and the instrument. The response of any transducer is highly dependent on how it its pulsed. Changing pulse energy, type (spike, square wave, or tone burst), and damping, as well as receiver gain and filtering, will have a significant effect on the excitation pulse ringdown envelope and hence on dead zone length.

As others have suggested, your best approach is to simply measure it under your actual test conditions using appropriate reference blocks.

----------- Start Original Message -----------
: Dear Friends,
: Dead zone is a property of probe.So far I know it's not the property of instrument.Dead zone is the difference between electrical zero and real zero. Calculation may be very difficult unless having the step blocks.
: Further informations are awaited related to the above.I'll be glad to know if there is any formulae for this.
: Thanks,
:
: Debdutta Mallik
------------ End Original Message ------------

Joe Buckley
Consultant, ASNT L-III, Honorary Secretary of BINDT
Level X NDT, BINDT, United Kingdom, Joined Oct 1999, 526

Joe Buckley

Consultant, ASNT L-III, Honorary Secretary of BINDT
Level X NDT, BINDT,
United Kingdom,
Joined Oct 1999
526
05:36 Apr-18-2007
I think there is a lot of confusion here, but Tom is absolutely correct.

The point which needs to be stressed is that Dead Zone is not something that could be calculated. It is the RESULT of a large number of factors, some of which will be difficult or impossible to measure/estimate. So the only valid approach is an empirical measurement, which will then apply only to the probe, instrument and test material combination.
Joe

----------- Start Original Message -----------
: Dead zone -- the interval following the excitation pulse in which potential exchoes are obscured by ringdown -- is a property of BOTH the probe and the instrument. The response of any transducer is highly dependent on how it its pulsed. Changing pulse energy, type (spike, square wave, or tone burst), and damping, as well as receiver gain and filtering, will have a significant effect on the excitation pulse ringdown envelope and hence on dead zone length.
: As others have suggested, your best approach is to simply measure it under your actual test conditions using appropriate reference blocks.
: : Dear Friends,
: : Dead zone is a property of probe.So far I know it's not the property of instrument.Dead zone is the difference between electrical zero and real zero. Calculation may be very difficult unless having the step blocks.
: : Further informations are awaited related to the above.I'll be glad to know if there is any formulae for this.
: : Thanks,
: :
: : Debdutta Mallik
------------ End Original Message ------------

Larry Mullins , E-mail:
Larry Mullins , E-mail:
06:27 Apr-18-2007
Lest we forget, we need to throw in surface roughness, interface shape (e.g. concave/convex) and couplant thickness / variability. Crunch those numbers if you dare! I'm with Tom and Joe.

----------- Start Original Message -----------
: I think there is a lot of confusion here, but Tom is absolutely correct.
: The point which needs to be stressed is that Dead Zone is not something that could be calculated. It is the RESULT of a large number of factors, some of which will be difficult or impossible to measure/estimate. So the only valid approach is an empirical measurement, which will then apply only to the probe, instrument and test material combination.
: Joe
: : Dead zone -- the interval following the excitation pulse in which potential exchoes are obscured by ringdown -- is a property of BOTH the probe and the instrument. The response of any transducer is highly dependent on how it its pulsed. Changing pulse energy, type (spike, square wave, or tone burst), and damping, as well as receiver gain and filtering, will have a significant effect on the excitation pulse ringdown envelope and hence on dead zone length.
: : As others have suggested, your best approach is to simply measure it under your actual test conditions using appropriate reference blocks.
: : : Dear Friends,
: : : Dead zone is a property of probe.So far I know it's not the property of instrument.Dead zone is the difference between electrical zero and real zero. Calculation may be very difficult unless having the step blocks.
: : : Further informations are awaited related to the above.I'll be glad to know if there is any formulae for this.
: : : Thanks,
: : :
: : : Debdutta Mallik
------------ End Original Message ------------

Debdutta Mallik
Consultant,
Malaysia, Joined Jun 2005, 37

Debdutta Mallik

Consultant,
Malaysia,
Joined Jun 2005
37
00:44 Apr-20-2007
Yes I agree with Tom and you also. Its a result of lot of factors related to instrment,probe etc and it cant be calculated on paper.

Regards,

Debdutta Mallik

Dhirender Singh , E-mail:
Dhirender Singh , E-mail:
01:30 Apr-20-2007
It is determined by the characteristics of search unit, the ultrasonic instrumentation, and the test object.

---------- Start Original Message -----------
: DEAR FRIEND,
: FOR PRACTICAL DEAD ZONE CALCULATION,YOU CAN USE OF V1 BLOCK IN
: AREA NEAR TO 50 mm DIA. PERSPEX .
: ---- Start Original Message -----------
: : Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: : Thanks
------------ End Original Message ------------

constant chuma , E-mail:
constant chuma , E-mail:
00:15 Apr-23-2007
----------- Start Original Message -----------
: The dead zone is measured for each system (transducer+cable+instrument) separately. And it would depend on the instrument gain and the required registration level (in terms of artificial flaw dimensions) for the given task. If you try to calculate it theoretically, the result may be very far away from the reality.
: Is it possible that you need to calculate the near field length? excuse me for the question if this is not the case, but I saw many examples of these 2 terms misinterpreted.
:
: : Could anyone explain how to calculate the dead zone on particular material for the Straight beam inspection. I understand it vary with transducer/instrument . What could be the general way how getting its extent.
: : Thanks
------------ End Original Message ------------

Lucy McDuff
Lucy McDuff
06:39 Sep-14-2007
----------- Start Original Message -----------
: Lest we forget, we need to throw in surface roughness, interface shape (e.g. concave/convex) and couplant thickness / variability. Crunch those numbers if you dare! I'm with Tom and Joe.
: : I think there is a lot of confusion here, but Tom is absolutely correct.
: : The point which needs to be stressed is that Dead Zone is not something that could be calculated. It is the RESULT of a large number of factors, some of which will be difficult or impossible to measure/estimate. So the only valid approach is an empirical measurement, which will then apply only to the probe, instrument and test material combination.
: : Joe
: : : Dead zone -- the interval following the excitation pulse in which potential exchoes are obscured by ringdown -- is a property of BOTH the probe and the instrument. The response of any transducer is highly dependent on how it its pulsed. Changing pulse energy, type (spike, square wave, or tone burst), and damping, as wellas receiver gain and filtering, will have a significant effect on the excitation pulse ringdown envelope and hence on dead zone length.
: : : As others have suggested, your best approach is to simply measure it under your actual test conditions using appropriate reference blocks.
: : : : Dear Friends,
: : : : Dead zone is a property of probe.So far I know it's not the property of instrument.Dead zone is the difference between electrical zero and real zero. Calculation may be very difficult unless having the step blocks.
: : : : Further informations are awaited related to the above.I'll be glad to know if there is any formulae for this.
: : : : Thanks,
: : : :
: : : : Debdutta Mallik
------------ End Original Message ------------

Ha ha, very clever Mr. Mullins, but you haven't contributed an answer.

Product Spotlight

#### CIVA 2020 UT Module

CIVA NDE Simulation Software is the world leader of NDT Simulation. The UT simulation Module incl
...
udes: - "Beam computation": Beam propagation simulation - "Inspection Simulation": Beam interaction with flaws or specimens The user can simulate a whole inspection process (pulse echo, tandem or TOFD) with a wide range of probes (conventional, Phased- arrays or EMAT), components, and flaws.
>

#### Lyft™: Pulsed Eddy Current Reinvented

PEC Reinvented—CUI Programs Redefined Corrosion under insulation (CUI) is possibly the greatest u
...
nresolved asset integrity problem in the industry. Current methods for measuring wall thickness with liftoff, without removing insulation, all have severe limitations. Eddyfi introduces Lyft — a reinvented, high-performance pulsed eddy current (PEC) solution. The patent- pending system features a state-of-the-art portable instrument, real- time C-scan imaging, fast data acquisition with grid-mapping and dynamic scanning modes, and flexibility with long cables. It can also scan through thick metal and insulation, as well as aluminum, stainless steel, and galvanized steel weather jackets. Who else but Eddyfi to reinvent an eddy current technique and redefine CUI programs. Got Lyft?
>

#### FD800 Bench Top Flaw Detectors

The bench-top FD800 flaw detector range combines state-of-the-art flaw detection with advanced mater
...
ial thickness capabilities. Designed for use in the laboratory these gauges are the tool you need for all your flaw detecting needs.
>

#### HARDNESS TESTER TKM-459CE combi

TKM-459CE combi applies 2 methods of hardness control: UCI and Leeb. It provides high-accuracy tes
...
ting of metals and alloys as well as items of different sizes and configurations, their hardened layers and galvanic coatings. Device represents results in HB, HRC, HV and others. Shock-, dust- and water-proof housing with intuitive software make this gauge easy to use in all working conditions.
>

Share...
We use technical and analytics cookies to ensure that we will give you the best experience of our website - More Info
Accept
top
this is debug window