PubMed · 14605549
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Rocco Orlando. 2003. Ventilators: how clever, how complex?. https://doi.org/10.1097/01.ccm.0000096412.07597.0e
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OBJECTIVES: To evaluate the force required to radially compress ureteral stents and the impact of compression on stent performance across a broad range of stent sizes and manufacturers. METHODS: Fourteen ureteral stents ranging in size from 6F to 10.3F were evaluated for radial compression using an MTS Micro Bionix Testing System using Testworks II software, 5N load cell, vibration isolation table, and socket set screws with rounded caps. Radial compression was exerted in 0.2-mm increments. Cycles of compression and a 100-second hold time were repeated for each stent to maximal compression. Three trials were completed for each stent. The Young's Modulus, E, was calculated from each trial using the engineering stress. Simultaneous flow data using normal saline were collected for the Amplatz stent. RESULTS: The Cook C-Flex (E = 30,355 +/- 910 Pa), Microvasive Percuflex Plus 6F (E = 28,973 +/- 250 Pa), Cook EndoSof (E = 28,403 +/- 471 Pa), and Fossa Open Lumen (E = 28,627 +/- 5,338) were the most resistant to compression and the Cook Amplatz 10.2F (E = 11,922 +/- 220 Pa) and Microvasive Percuflex Plus 10.3F (E = 8,247 +/- 286 Pa) were the least resistant to compression. Stress relaxation occurred similarly in all stents. Flow through the Cook Amplatz stent decreased at a rate of 5 mL/s/mm of compression linearly (R2 = 0.95). CONCLUSIONS: Stents resistant to radial compression are critical for function in the face of extrinsic ureteral obstruction. The Cook C-Flex ureteral stent resisted extrinsic compressive forces best. Although large-lumen stents are often used in this clinical situation, they were the most susceptible to compressive forces.
A birdcage coil capable of operating simultaneously and independently in three orthogonal dimensions has been developed. A co-rotational end-ring mode producing an RF field in the longitudinal direction was utilized in addition to the two common transverse orthogonal modes. Two conductor turns were used for each of the coil's windows, increasing its inductance by a factor of four, thereby, making the coil suitable for low-frequency applications. Two or three-frequency detection can be easily carried out with this device. Orthogonality of the coil's channels allows arbitrarily close frequency positioning of each resonant mode, potentially useful in wide-line NQR studies, in which simultaneous excitation/detection of signals from three adjacent regions of a single wide line can be performed. The coil's performance was evaluated using a three-dimensional scheme, in which a circularly polarized experiment was combined with a linearly polarized measurement at another frequency, resulting in SNR improvement by 55%.
Optical tomography of gel dosimeters is a promising and cost-effective avenue for quality control of radiotherapy treatments such as intensity-modulated radiotherapy (IMRT). Systems based on a laser coupled to a photodiode have so far shown the best results within the context of optical scanning of radiosensitive gels, but are very slow ( approximately 9 min per slice) and poorly suited to measurements that require many slices. Here, we describe a fast, three-dimensional (3D) optical computed tomography (optical-CT) apparatus, based on a broad, collimated beam, obtained from a high power LED and detected by a charged coupled detector (CCD). The main advantages of such a system are (i) an acquisition speed approximately two orders of magnitude higher than a laser-based system when 3D data are required, and (ii) a greater simplicity of design. This paper advances our previous work by introducing a new design of focusing optics, which take information from a suitably positioned focal plane and project an image onto the CCD. An analysis of the ray optics is presented, which explains the roles of telecentricity, focusing, acceptance angle and depth-of-field (DOF) in the formation of projections. A discussion of the approximation involved in measuring the line integrals required for filtered backprojection reconstruction is given. Experimental results demonstrate (i) the effect on projections of changing the position of the focal plane of the apparatus, (ii) how to measure the acceptance angle of the optics, and (iii) the ability of the new scanner to image both absorbing and scattering gel phantoms. The quality of reconstructed images is very promising and suggests that the new apparatus may be useful in a clinical setting for fast and accurate 3D dosimetry.