PubMed Health⌕ Search

PubMed · 977278

A rocking motion sensor for the blind.

Abstract

Rocking motion is an unconscious and often unwanted phenomenon exhibited by the blind. It is usually manifested in oscillatory back and forth, side to side, or rotatory movements of the upper torso or head at about 1 Hz rate. Subjects desiring to function unobtrusively in the world of the sighted need to be alerted when rocking so they can control it. The rocking motion sensor incorporates biofeedback and records rock occurrences. A miniature body mounted accelerometer senses body accelerations exceeding 0.1g. These motions during a given period, compared with a presettable "rock threshold", discriminate rocking from normal activities. Sound biofeedback alerts the subject that he has exceeded threshold. Another counting and timing subsystem determines "end of rock" and resets the system. A recorder is provided that records signals only during rocking. Timing information is provided on a separate channel to permit later time line analysis. The rocking motion sensor system utilizes primarily solid state CMOS circuits with a combination of synchronous-asynchronous timing. The recorder is a modified commercial unit. The two units are separate, portable, and belt mounted. Tests have been made and results will be presented.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

J T Polhemus, J E Morgan, A Mandell. 1976. A rocking motion sensor for the blind.. https://pubmed.ncbi.nlm.nih.gov/977278/

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related citations

Optimal design of non-Newtonian, micro-scale viscous pumps for biomedical devices.

The present paper addresses the numerical optimization of geometrical parameters of non-Newtonian micro-scale viscous pumps for biomedical devices. The objective is to maximize the mass flow rate per unit of shaft power consumed by the rotor when an external pressure load is applied along the channel that houses the rotor. Two geometric parameters are considered in the optimization process: (i) the height of the channel that houses the rotor (H) and (ii), the eccentricity (epsilon) of the rotor. Three different micro-scale viscous pump configurations were tested: a straight-housed pump (I-shaped housing) and two curved housed pumps (L- and U-shaped housings). The stress-strain constitutive law is modeled by a power-law relation. The results show that the geometric optimization of micro-scale viscous pumps is critical since the mass flow rate propelled by the rotor is highly dependent on epsilon and H. Numerical simulations indicate that mass flow rate is maximized when epsilon approximately 0, namely when the rotor is placed at a distance of 0.05 radii from the lower wall. The results also show that micro-scale viscous pumps with curved housing provide higher mass flow rate per unit of shaft power consumed when compared with straight-housed pumps. The results are presented in terms optimized dimensions of all three configurations (i.e., H(opt) and epsilon(opt)) and for values of the power-law index varying between 0.5 (shear thinning fluids) and 1.5 (shear-thickening fluids).

Biomedical Engineering↗