
This technique is used for the detection of internal and surface                  (particularly distant surface) defects in sound conducting materials.
                   
The                  principle is in some respects similar to echo sounding. A short                  pulse of ultrasound is generated by means of an electric charge                  applied to a piezo electric crystal which vibrates for a very                  short period at a frequency related to the thickness of the crystal.                  In flaw detection this frequency is usually in the range of one                  million to six million times per second (1 MHz to 6 MHz). Vibrations                  or sound waves at this frequency have the ability to travel a                  considerable distance in homogeneous elastic material, such as                  many metals, with little attenuation. The velocity at which these                  waves propagate is related to the 'Youngs Modulus' for that material                  and is characteristic of that material. For example the velocity                  in steel is 5900 metres per second, and in water 1400 metres per                  second.
                   
Ultrasonic                  energy is considerably attenuated in air, and a beam propagated                  through a solid will, on reaching an interface (e.g. a defect,                  or intended hole, or the backwall) between that material and air,                  reflect a considerable amount of energy in the direction equal                  to the angle of incidence.
                   
For                  contact testing the oscillating crystal is incorporated in a hand                  held probe which is applied to the surface of the material to                  be tested. To facilitate the transfer of energy across the small                  air gap between the crystal and the test piece, a layer of liquid,                  usually oil, water or grease, is applied to the surface.
                   
As                  mentioned previously, the crystal does not oscillate continuously                  but in short pulses, between each of which it is quiescent. Piezo                  electric materials not only convert electri-cal pulses to mechanical                  oscillations, but will also transduce mechanical oscillations                  into electrical pulses; thus we have not only a generator of sound                  waves but also a detector of returned pulses. The crystal is in                  a state to detect returned pulses when it is quiescent. The pulse                  takes a finite time to travel through the material to the interface                  and to be reflected back to the probe.
                   
The                  normal method of presenting information in ultrasonic testing                  is by means of a cathode ray tube, in which horizontal movement                  of the spot from left to right represents time elapsed. The rate                  at which the spot moves is such that it gives the appearance of                  a horizontal line on the screen. The system is synchronised electronically                  so that at the instant the probe receives its electrical pulse                  the spot begins to traverse the screen. An upward deflection (peak)                  of the line on the left hand side of the screen is an indication                  of this occurrence. This peak is usually termed the initial pulse.
                   
Whilst                  the base line is perfectly level the crystal is quiescent. Any                  peaks to the right of the initial pulse indicate that the crystal                  has received an incoming pulse reflected from one or more interfaces                  in the material. Since the spot moves at a very even speed across                  the tube face, and the pulse of ultrasonic waves moves at a very                  even velocity through the material, it is possible to calibrate                  the horizontal line on the screen in terms of absolute measurement.                  The use of a calibration block, which produces a reflection from                  the back wall a known distance away from the crystal together                  with variable controls on the flaw detector allows the screen                  to be calibrated in units of distance, and therefore determination                  of origins of returned pulses obtained from a test piece.
                   
It                  is therefore possible not only to discover a defect between the                  surface and the back wall, but also to measure its distance below                  the surface. It is important that the equipment is properly calibrated                  and, since it is in itself not able to discriminate between intended                  boundaries of the object under test and unintended discontinuities,                  the operator must be able to identify the origin of each peak.                  Further as the pulses form a beam it is also possible to determine                  the plan position of a flow.
                   
The                  height of the peak (echo) is roughly proportional to the area                  of the reflector, though there is on all instruments a control                  which can reduce or increase the size of an indication - variable                  sensitivity in fact. Not only is part of the beam reflected at                  a material/air interface but also at any junction where there                  is a velocity change, for example steel/slag in a weld.
                   
Probing                  all faces of a test piece not only discovers the three dimensional                  defect and measures its depth, but can also determine its size.                  Two dimensional (planar) defects can also be found but it is best                  that the incident beam impinges on the defect as near to right                  angles to the plane as possible. To achieve this some probes introduce                  the beam at an angle to the surface. In this manner longitudinal                  defects in tubes (inner or outer surface) are detected.
                   
Interpretation                  of the indications on the cathode ray tube requires a certain                  amount of skill, particularly when testing with hand held probes.                  The technique is, however, admirably suited to automatic testing                  of regular shapes by means of a monitor - an electronic device                  which fits into the main equipment to provide an electrical signal                  when an echo occurs in a particular position on the trace. The                  trigger level of this signal is variable and it can be made to                  operate a variety of mechanical gates and flaw warnings.
                   
Since                  the velocity of sound in any material is characteristic of that                  material, it follows that some materials can be identified by                  the determination of the velocity. This can be applied, for example                  in S.G. cast irons to determine the percentage of graphite nodularity.                  This process can also be automated and is now in use in many foundries.                  A typical equipment is the 'Qualiron'.
                   
When                  the velocity is constant, as it is in a wide range of steels,                  the time taken for the pulse to travel through the material is                  proportional to its thickness. Therefore, with a properly calibrated                  instrument, it is possible to measure thickness from one side                  with an accuracy in thousandths of an inch. This technique is                  now in very common use. A development of the standard flaw detector                  is the digital wall thickness gauge. This operates on similar                  principles but gives an indication, in LED or LCD numerics, of                  thickness in absolute terms of millimetres. These equipments are                  easy to use but require prudence in their application.
                   
Advantages                  of Ultrasonic Flaw Detection:
                   
- Thickness                    and lengths up to 30 ft can be tested.  
 - Position,                    size and type of defect can be determined.  
 - Instant                    test results.  
 - Portable.                     
 - Extremely                    sensitive if required.  
 - Capable                    of being fully automated.  
 - Access                    to only one side necessary.  
 - No                    consumables.  
 
                   
Disadvantages                  of Ultrasonic Flaw Detection:
                   
- Indications                    require interpretation (except for digital wall thickness gauges).                     
 - Considerable                    degree of skill necessary to obtain the fullest information                    from the test.  
 - Very                    thin sections can prove difficult.  
 
                   
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