Orientation imaging using spatially resolved acoustic spectroscopy (SRAS) Steve D. Sharples, Wenqi Li, Richard Smith, Matt Clark and Mike Somekh Applied Optics Group, Electrical Systems & Optics Research Division Faculty of Engineering, University of Nottingham. AFPAC, January 2011 What is SRAS? EBSD image courtesy of University of Wales, Swansea SRAS surface acoustic wave velocity image Spatially Resolved Acoustic Spectroscopy A Laser ultrasound technique for imaging microstructure** Uses SAW velocity as contrast - varies with grain orientation varies with SAW direction Produces nice images of grains and tells us how they are orientated Tells us all sorts of nice information about the sample microstructure f-SRAS: frequency spectrum SRAS Excite with short (ns) laser pulses projected through optical grating. The grating generates narrowband SAWs. Only one wavelength, λ (the grating period). Detect the SAWs with a broadband optical detector. Measure the frequency on a scope. Use v = f λ to get the velocity The patch under the grating is the patch which is measured f-SRAS: taking a velocity measurement A few nice pictures… Austenitic stainless steel weld L-R Austenitic stainless steel weld U-D Example images showing the capabilities of SRAS: Scalability from large to small (titanium alloy) 84mm 10mm Resolution: 400μm Resolution: 400μm Resolution: 25μm ms-1 108μm 700μm Resolution: 25μm What’s new since last AFPAC? 1. Instrumentation A dedicated SRAS microscope Smaller, much faster, cheaper, simpler Will have ability to scan on “rough surfaces” next month! Higher spatial resolution 2. Determination of orientation from SAW velocities cubic crystals (e.g. nickel, aluminium) (1) 3rd generation SRAS instrument New dedicated SRAS system funded by emda (East Midlands Development Agency). Completion due April 2011. Smaller, faster, more capable Example images from new instrument (1) Ti-6Al-4V 170x80mm 25x250μm pixel size 2.2 megapixels 48 minutes scan time >750 points/sec Example images from new instrument (2) (2) From “contrast” to orientation measurement The velocity depends on the crystallographic orientation Ok to go from orientation to velocity (forward) Trickier to invert this problem So… Solve the forward problem v=f( orientation ) Fit the data to the forward problem to find the orientation Forward model: calculating SAW velocities from known orientation and known elastic constants Define elastic constants, and multiply by rotation matrix Define propagation direction l1, l2 and velocities substitute into |jk-jkv2| = 0 l1, l2 = propagation direction = density V = phase velocity choose the 3 lower half plane roots of l3 and its 3 C = stiffness tensors plot the curve of |d mn |= |cm3klk(n)ll(n) | vs. velocities jk = lillcijkl choose the minima of |d mn | to determine velocities d mn = determinant of |jk-jkv2| calculate the out of plane displacement of velocities 3 = eigenvectors of displacement First the forward problem for cubic Nickel SAW velocity as a function of orientation: cubic crystal: Nickel Propagation in multiple directions – single crystal Ni Fit analytic curves to data to get orientation Getting the orientation… Analytically calculated velocity as a function of orientation + Measure velocity as a function of propagation direction on surface + Simple fitting algorithm = Orientation of the crystals Propagation in multiple directions – single crystal Ni Orientation imaging on nickel Supposedly “single crystal” nickel, actually consists of two large grains SAW velocity left-right SRAS: Conclusions SRAS is faster and fancier than ever before! We got a nice new machine thanks to EMDA It will have optically rough surface capability shortly We can go from measurement to orientation Next: More forward modelling Slicker fitting Strategies for speed vs information Higher resolution Acknowledgements Steve Sharples Wenqi Li Richard Smith RCNDE EMDA RR Aeroengines EPSRC University of Wales (Swansea) For more information or if you have an interesting sample, please email: steve.sharples@nottingham.ac.uk