Difficult to penetrate materials square wave pulser GE Inspection Technologies Jim Costain August 2009 Why do we have difficult-to-penetrate materials ? Ultrasound is subject to attenuation due to different effects Attenuation Absorption Diffusion Divergence Internal friction X Heat X Frequency X X X Grain size X Test Frequency is linked to attenuation 2/ GE / The energy chain The more energy we send into the material, the better chance we have to go through it • Where can we influence the energy sent to the material ? Probe selection Pulser type and pulser setting Material to probe interface 3/ GE / Material - Probe interface We can improve energy conduction from the probe to the material • Optimization of probe surface • Optimization of coupling quality • Optimization of probe selection (acoustic impedance of the contact face ) 4/ GE / Piezocomposite probes give you higher electroacoustic efficiency Piezocomposites materials provide > A high pulse amplitude for good penetration through the test object with a good signal to noise ratio > A shorter acoustic pulse duration for a good axial resolution > A lower acoustic impedance (ideal for coupling wedges and delay lines) 5/ GE / • The lower the frequency, the thicker the piezoelectric Volume Piezoelectric volume in function of frequency • Low frequency probes typically have larger diameters MHz 10 7.5 5 3.5 4 2 2.25 0.5 1 Low frequency probes need more energy to enter in oscillation 6/ GE / Square Wave Pulsers - Spike Pulsers The pulser’s setting is related to the application 80 • Square wave pulsers produce better results when the probe frequency is lower or equal at 2 MHz 75 70 65 60 55 50 0,5 MHz Square wave pulser have to be preferred below 2MHz 1 MHz 2 MHz 4 MHz 10 MHz Spike pulser (*) Square Wave pulser (*) (*) Comparisons realized with USD 15SX & USD 15SQ 7/ GE / Spike excitation and the probe response Low frequency probes • They usually have big diameters • Thick crystals →They need more energy If the pulse length is too short, the element doesn’t oscillate at the maximum amplitude Spike Pulser with a 2 MHz 1’ probe →The excitation is too weak 8/ GE / Square wave excitation and the probe response Up to 450 Volts Up to 1000ns pulse width Correct pulse length, The element is exactly excited at resonance. →This is the optimum setting 9/ GE / Square wave excitation and the probe response. If the Pulse length is too long, Element oscillation is distorted and extends in time →Distortion. →Double pulse. 10 / GE / The instrument and its pulser How to avoid wrong pulser adjustment ? • For day to day applications, use the “Spike” mode of your flaw detector • Use Energy and damping to optimize penetration and resolution • For more difficult applications (highly attenuative materials), optimize • Voltage • Pulse width of the “square wave” mode of your flaw detector 11 / GE / Optimum pulse width determination • The pulse width can be calculated with the following formula • It can also be optimized manually Maximize amplitude of echo using the pulse width parameter 12 / GE / Conclusion • The Square wave pulser is very useful for thick and highly attenuative material using low frequency transducers • Can improve penetration and signal to noise ratio on thick or attenuative materials • Optimized usage at or below 2Mhz but can be used with care at 4Mhz 13 / GE / Thank you 14 / GE /