Dotted-line FLEET for two-component velocimetry.

Femtosecond laser electronic excitation tagging (FLEET) is a powerful unseeded velocimetry technique typically used to measure one component of velocity along a line, or two or three components from a dot. In this Letter, we demonstrate a dotted-line FLEET technique which combines the dense profile capability of a line with the ability to perform two-component velocimetry with a single camera on a dot. Our set-up uses a single beam path to create multiple simultaneous spots, more than previously achieved in other FLEET spot configurations. We perform dotted-line FLEET measurements downstream of a highly turbulent, supersonic nitrogen free jet. Dotted-line FLEET is created by focusing light transmitted by a periodic mask with rectangular slits of 1.6 × 40 mm2 and an edge-to-edge spacing of 0.5 mm, then focusing the imaged light at the measurement region. Up to seven symmetric dots spaced approximately 0.9 mm apart, with mean full-width at half maximum diameters between 150 and 350 µm, are simultaneously imaged. Both streamwise and radial velocities are computed and presented in this Letter.

Multi-line FLEET by imaging periodic masks.

A simple linear configuration for multi-line femtosecond laser electronic excitation tagging (FLEET) velocimetry is used for the first time, to the best of our knowledge, to image an overexpanded unsteady supersonic jet. The FLEET lines are spaced 0.5-1.0 mm apart, and up to six lines can be used simultaneously to visualize the flowfield. These lines are created using periodic masks, despite the mask blocking 25%-30% of the 10 mJ incident beam. Maps of mean single-component velocity in the direction along the principal flow axis, and turbulence intensity in that same direction, are created using multi-line FLEET, and computed velocities agree well with those obtained from single-line (traditional) FLEET. Compared to traditional FLEET, multi-line FLEET offers increased simultaneous spatial coverage and the ability to produce spatial correlations in the streamwise direction. This FLEET permutation is especially well suited for short-duration test facilities.

Data indicating temperature response of Ti-6Al-4V thin-walled structure during its additive manufacture via Laser Engineered Net Shaping.

An OPTOMEC Laser Engineered Net Shaping (LENS(™)) 750 system was retrofitted with a melt pool pyrometer and in-chamber infrared (IR) camera for nondestructive thermal inspection of the blown-powder, direct laser deposition (DLD) process. Data indicative of temperature and heat transfer within the melt pool and heat affected zone atop a thin-walled structure of Ti-6Al-4V during its additive manufacture are provided. Melt pool temperature data were collected via the dual-wavelength pyrometer while the dynamic, bulk part temperature distribution was collected using the IR camera. Such data are provided in Comma Separated Values (CSV) file format, containing a 752×480 matrix and a 320×240 matrix of temperatures corresponding to individual pixels of the pyrometer and IR camera, respectively. The IR camera and pyrometer temperature data are provided in blackbody-calibrated, raw forms. Provided thermal data can aid in generating and refining process-property-performance relationships between laser manufacturing and its fabricated materials.

Deep tendon reflexes: a study of quantitative methods.

OBJECTIVE: The deep tendon reflex (DTR) is routinely used by clinicians to evaluate the nervous system. Depressed and hyperactive DTRs suggest peripheral and central nervous system compromise, respectively. Limitations of DTRs are: qualitative nature of the assessments based upon subjective grading, and limited inter-rater reliability. This preliminary study was undertaken to quantify the tendon tap used by clinicians to elicit DTRs and the reflex response elicited. METHODS: Tendon taps were applied to a force transducer in hypo-, normo-, and hyperreflexic ranges by 2 clinicians, using 3 different tendon hammers (Babinski, Queen Square, and Taylor). Patellar DTRs, measured as joint angle excursion with an electrogoniometer, were compared in hyper- and normoreflexic individuals. RESULTS: Median peak tap force was 1 2.8, 38.0, and 85.2 Newtons (Nt), respectively, for eliciting hyper-, normo-, and hyporeflexic DTRs. Peak tap force was similar in the hyper- and normoreflexic ranges for all 3 hammers; in the hyporeflexic range, peak tap forces with the Taylor hammer were lower. A good distinguishing feature between hyper- and normoreflexic patellar DTRs was briskness, measured as the quotient of knee excursion divided by peak tendon tap force. Knee excursion is a non-linear patellar DTR response, when measured sitting. CONCLUSIONS: Peak tap forces used by clinicians fall into 3 ranges: 0-20 Nt for hyperreflexia, 21-50 Nt for normoreflexia, and >50 Nt for hyporeflexia. The Taylor hammer, with small mass and short handle, has a ceiling effect in the hyporeflexic range. We propose a systematic method for DTR testing.