Difference between revisions of "SRAS for materials characterisation"

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(EMDA Sponsored Instrument)
(EMDA Sponsored Instrument)
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This approach allows the determination of the velocity for each laser pulse. This makes the data acquisition very fast. The laser in the EMDA system fires 6000 times a second, so we can take 6000 velocity measurements per second. Real scanning rates, which include the movement of stages, data downloading etc, reduce this rate to ~1200 points/second. This is 100 times faster than previous generations of instrument.
 
This approach allows the determination of the velocity for each laser pulse. This makes the data acquisition very fast. The laser in the EMDA system fires 6000 times a second, so we can take 6000 velocity measurements per second. Real scanning rates, which include the movement of stages, data downloading etc, reduce this rate to ~1200 points/second. This is 100 times faster than previous generations of instrument.
  
The EMDA instrument can also generate waves in any arbitrary direction by rotating the mask pattern The detection spot can also be moved by use of a computer controlled mirror. this allows for velocity surface measurements or velocity vector maps to be produced with the need to rotate the sample.
+
The EMDA instrument can also generate waves in any arbitrary direction by rotating the mask pattern The detection spot can also be moved by use of a computer controlled mirror. this allows for velocity surface measurements or velocity vector maps to be produced with the need to rotate the sample. The instrument is being upgraded to cope with optically rough surfaces which will allow scanning to take place on more industrially relevant samples.
  
 
The instrument has exceptional spatial resolution and working frequency ranges. Routine scans have been performed from 100-300 MHz with spatial resolution better than 50 microns/pt. With this resolution it is possible to see very fine details in material structure.  
 
The instrument has exceptional spatial resolution and working frequency ranges. Routine scans have been performed from 100-300 MHz with spatial resolution better than 50 microns/pt. With this resolution it is possible to see very fine details in material structure.  

Revision as of 09:12, 14 April 2011

What is SRAS

SRAS System.PNG
SRAS 300dpi emda sras.pngSRAS 300dpi sras austenitic ss.png

SRAS stands for Spatially Resolved Acoustic Spectroscopy, it is a technique for mapping the surface acoustic wave velocity of a material. The technique is analogous to optical spectroscopy techniques where analysis of the optical spectrum and the wavelengths that are most readily transmitted or absorbed tells us some properties of the sample being examined. In the acoustic sense we monitor the spectrum of sound waves emitted from a grating source. The technique can be performed two ways, the first is to use a fixed frequency source and sweep the grating spacing or the grating period can be fixed and the frequency is swept.

To measure the acoustic spectrum at each point on the sample a fixed grating is illuminated with a short laser pulse (typically ~1ns). As the laser pulse contains a broad range of frequencies, only the frequencies which match the grating spacing and acoustic velocity of that sample point will be generated. We measure the waves that have been generated close to the excitation region (see top figure). We can then calculate the frequencies generated and with the knowledge of the grating spacing we can obtain the acoustic velocity using v = fλ. If the sample is raster scanned we build up a detailed image of the sample velocity for that propagation direction. These images show the grain structure of the material and are very useful for material scientists for assessing the properties of the material.


EMDA Sponsored Instrument

EMDA System.jpg EMDA Ti LG685.png
CCD Fringes x10.PNG
TiLG685 zoom2 300 4.png

The EMDA instrument is the most advanced version of SRAS instrumentation we have at Nottingham. This instrument has been developed to provide rapid velocity imaging on a variety of surface finishes.

The instrument uses a fixed grating, projecting a pattern of stripes onto the sample. These stripes define the wavelength of the generated acoustic waves. The mask is illuminated with a short pulse of laser light ~1ns, the mask acts as a filter and so only sound waves with the frequency to match the fixed wavelength and the velocity of the material under the patch are generated. We detected the generated waves close to the generation region. We determine the velocity by looking at the frequency of the waves we detect and our knowledge of the mask spacing.

This approach allows the determination of the velocity for each laser pulse. This makes the data acquisition very fast. The laser in the EMDA system fires 6000 times a second, so we can take 6000 velocity measurements per second. Real scanning rates, which include the movement of stages, data downloading etc, reduce this rate to ~1200 points/second. This is 100 times faster than previous generations of instrument.

The EMDA instrument can also generate waves in any arbitrary direction by rotating the mask pattern The detection spot can also be moved by use of a computer controlled mirror. this allows for velocity surface measurements or velocity vector maps to be produced with the need to rotate the sample. The instrument is being upgraded to cope with optically rough surfaces which will allow scanning to take place on more industrially relevant samples.

The instrument has exceptional spatial resolution and working frequency ranges. Routine scans have been performed from 100-300 MHz with spatial resolution better than 50 microns/pt. With this resolution it is possible to see very fine details in material structure.

All these capabilities have been constructed into a compact head that can be mounted above a scanning system, as picutred, or mounted directly to a scanning head. The dimensions are approximately 350x200x150 mm with an umbilical connection to a rack containing the computer and other electronics.



From Velocity to Orientation

description of going from velocity contrast images to orientation.

SRAS 300dpi al 011 111.png
SRAS 300dpi nickel 001 011 111.png



History of the technique

description of k sras and older instruments

Related publications