1887
banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Compact system for high-speed velocimetry using heterodyne techniques
Rent:
Rent this article for
USD
10.1063/1.2336749
/content/aip/journal/rsi/77/8/10.1063/1.2336749
http://aip.metastore.ingenta.com/content/aip/journal/rsi/77/8/10.1063/1.2336749
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

The basic geometry of a velocimeter using the heterodyne technique uses fiber optics to transport light from the laser to a probe that launches light to the moving surface.

Image of FIG. 2.
FIG. 2.

The heterodyne velocimeter is assembled from commercially available parts.

Image of FIG. 3.
FIG. 3.

The four-channel heterodyne system is packaged into a portable case. From top to bottom are the fiber laser, the custom fiber/detector chassis, and the high-bandwidth digitizer.

Image of FIG. 4.
FIG. 4.

(a) The beat wave form often shows amplitude fluctuations as the intensity of the light from the moving surface changes during the experiment. The individual beat cycles cannot be resolved with this time base. (b) Expanding the time base reveals the individual beat cycles. A measured period of corresponds to a velocity of .

Image of FIG. 5.
FIG. 5.

(a) The beat wave form obtained from an explosively driven metal shows both amplitude and base line variations. (b) The spectrogram was calculated with 1024-point Fourier transform windows. (c) The Fourier transform code allows the velocity vs time data to be extracted from the spectrogram.

Image of FIG. 6.
FIG. 6.

(a) The individual beat cycles can be seen in the early part of the beat wave forms on the cook-off experiment. (b) The velocity time histories span four decades.

Image of FIG. 7.
FIG. 7.

(a) For the gas gun experiment, the light from the heterodyne probe passed through two LiF windows. (b) The resulting spectrogram shows two discrete frequencies. (c) The Fourier transform code allows each velocity profile to be extracted separately.

Image of FIG. 8.
FIG. 8.

(a) The beat amplitude shows a slowly varying region as the elastic precursor arrives at the surface, and then a rapidly varying region once the actual shock arrives. (b) Fitting the shock arrival times to a sine wave yields residuals with a standard deviation among the six probes.

Loading

Article metrics loading...

/content/aip/journal/rsi/77/8/10.1063/1.2336749
2006-08-24
2014-04-17
Loading

Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Compact system for high-speed velocimetry using heterodyne techniques
http://aip.metastore.ingenta.com/content/aip/journal/rsi/77/8/10.1063/1.2336749
10.1063/1.2336749
SEARCH_EXPAND_ITEM