RESUMEN
BACKGROUND: Establishing a stand-alone cryogenic test stand is of vital importance to ensure the highly reliable and available operation of superconducting radio-frequency module in a synchrotron light source. Operating a cryogenic test stand relies strongly on a capability to deliver two-phase helium along long cryogenic transfer lines. A newly constructed cryogenic test stand with flexible cryogenic transfer lines of length 220 m at National Synchrotron Radiation Research Center is required to support a superconducting radio-frequency module operated at 126.0 kPa with a 40-W dynamic load for a long-term reliability test over weeks. It is designed based on a simple analytical approach with the introduction of a so-called tolerance factor that serves to estimate the pressure drops in transferring a two-phase helium flow with a substantial transfer cryogenic heat load. Tolerance factor 1.5 is adopted based on safety factor 1.5 commonly applied in cryogenic designs to estimate the total mass flow rate of liquid helium demanded. A maximum 60-W dynamic load is verified with experiment measured with heater power 60 W instead after the cryogenic test stand has been installed. RESULTS: Aligning the modeled cryogenic accumulated static heat load with the results measured in situ, actual tolerance factor 1.287 is obtained. The feasibility and validity of our simple analytical approach with actual tolerance factor 1.287 have been scrutinized by using five test cases with varied operating conditions. Calculated results show the discrepancies of the pressure drops between the estimated and measured values for both liquid helium and cold gaseous helium transfer lines have an underestimate 0.11 kPa and an overestimate 0.09 kPa, respectively. A discrepancy is foreseen, but remains acceptable for engineering applications from a practical point of view. CONCLUSIONS: The simple analytical approach with the introduction of a tolerance factor can provide not only insight into optimizing the choice of each lossy cryogenic piping element of the transfer lines in the design phase but also firm guidance for upgrading the present cryogenic transfer lines for its subsequent application.
RESUMEN
BACKGROUND: This retrospective study aimed to determine the factors leading to obstructive granulation tissue formation after the placement of a self-expandable metallic stent (SEMS) in patients with benign tracheal disease. METHODS: From 2001 to 2007, a total of 67 patients (age: 62.1 +/- 15.4 years; range: 23-87 years) with benign tracheal disease received 75 ultraflex SEMS in our institution. RESULTS: There were 35 SEMSs complicated by obstructive granulation tissue formation out of the 75 stents placed in patients with tracheal disease, giving an incidence of 47.8 % (32/67 patients). The median time until developing granulation tissue was 106 days (IQR, 46-396). Structural airway obstruction prior to SEMS implantation independently predicted obstructive granulation tissue formation after SEMS implantation (odds ratio: 3.84; 95 % CI: 1.01-8.7; P = 0.04). Time to granulation tissue detection was shorter in patients with structural airway obstruction before SEMS implantation (structural airway obstruction vs. dynamic collapse airway: median [IQR] 95 [38-224, n = 26] vs. 396 days [73-994, n = 9]; P = 0.02). CONCLUSIONS: Obstructive granulation tissue formation is not uncommon after SEMS implantation and structural airway obstruction prior to SEMS implantation is an independent predictor. Although SEMS implantation should be restricted to a select population, it may be placed in patients not suitable for surgical intervention or rigid bronchoscopy with anesthesia because of poor pulmonary function.