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1.
A new evaluation model for SK combinator expressions is presented and used as a basis for the design of a novel processor. The resulting machine architecture resembles a dataflow ring, but executions are constrained to be fully lazy. An automatic dynamic load sharing mechanism for a distributed multiprocessor architecture is suggested, and initial simulation results are presented. 相似文献
2.
A study was undertaken to examine the sensitivity of a wastewater population of coliphage, total coliforms and total flora present in raw sewage and secondary effluent after irradiating with similar doses delivered by a high-energy electron beam and y -radiation. The electron beam study was conducted on a large scale at the Virginia Key Wastewater Treatment Plant, Miami, Fla. The facility is equipped with a 1.5 MeV, 50 mA electron accelerator, with a wastewater flow rate of 8 ls−1. Concurrent y-radiation studies were conducted at laboratory scale using a 5000 Ci, 60Co y -source. Three logs reduction of all three test organisms were observed at an electron beam dose of 500 krads, while at least four logs reduction were observed at the same dose utilizing the y-source. 相似文献
3.
The effect of shear on floc properties was observed through population balance to comprehend the mechanisms of flocculation, in particular the role of restructuring. Little fundamental attention has been given before to the shear influence responsible for creating compact aggregates, while the floc characteristics might differ in other conditions. It is crucial to understand how aggregates evolve to steady state, if their properties are to be ‘tailored’ to suit subsequent solid-liquid separation. From a previous experimental study (Langmuir 18(6) (2002) 1974), restructuring was observed to occur extensively in the flocculation of latex particles in couette-flow, and was proposed to be responsible for the decrease in floc size on their transition to equilibrium. On the other hand, flocs of larger primary particles were more susceptible to breakage, with densification occurring as a result of fragmentation and re-aggregation. Denser flocs were found when structural deformation dominated, particularly in the initial stage of the process, while comparatively tenuous ones were observed when formation and breakage kinetics were the governing mechanisms. The distinct manners in which aggregates of different primary particle sizes evolved with time, were replicated with a population balance that incorporated the floc structural variation; verifying that restructuring indeed played a crucial role under certain flocculation conditions. 相似文献
4.
1 引言礁岩潮间带遍布全球 ,而日本最为多见。潮间带生长着大量的座生生物。由于海水流速常常超过10m·s- 1,这些座生生物常常受到巨大的侧向和向上拉力 ,所以座生生物在潮间带生存的必要条件是要有强大并且耐环境侵蚀的粘接能力。仔细查看一下潮间带礁岩表面就会发现许多种永久或半永久吸附其上的生物。藤壶、牡蛎、贻贝、笠贝、管栖性多毛纲生物和海带只是其中少数的几个例子。这类生物的粘接方式之所以引起人们的兴趣 ,是因为它们的粘接策略是随机应变 ,在水下它们可以与所遇到的任何类型的硬质表面 ,例如矿物、石蜡、聚丙烯酸酯、聚… 相似文献
5.
The literature on the spread and vaporisation of cryogenic liquids on water is reviewed and a new model proposed. The model incorporates the features o
Symbols | |
Cp | Heat capacity. |
g | Acceleration due to gravity. |
Gm | Molar vaporisation rate. |
h | Latent heat with two suffices denoting phase change. |
h | Pool thickness (no suffices). |
i | Enthalpy. |
k,K | Constants. |
KA,KB | Functions of pool temperature and composition. |
kw | Thermal diffusivity of water. |
l | Depth in water where temperature is constant. |
L | Length scale of an oil spill. |
Lm | Molar liquid spill rate. |
Lwi | Latent heat of fusion of ice. |
M | Pool mass, M0 initially. |
Ms,Mv | Mass spilled, mass vaporised. |
q | Heat flux to cryogenic liquid. |
r | Radial co-ordinate |
R,R* | Radius of pool. |
t | Time. |
T | Temperature. |
U | Velocity. |
Wm | Number of moles of material in the pool. |
xA | Molar methane portion of liquid pool (xB, ethane). |
xAS | Molar methane portion of spilling liquid. |
yA | Molar methane portion of vapour (yB, ethane). |
z | Vertical coordinate. |
δ | Vapour layer thickness. |
ΔT | Temperature difference. |
? | Ice layer thickness. |
θ | Temperature relative to freezing point of water. |
λ | Effective thermal conductivity. |
μ | Viscosity. |
? | Density. |
σ | Surface tension. |
ø | Heat flux to liquid pool = q. |
Suffices | |
A | Average (or methane fraction with x,y). |
B | Boiling point of cryogen (or ethane fraction with x,y). |
fc | Film collapse. |
fg | Liquid to vapour phase change. |
F | Freezing of water. |
i | Ice. |
l, L | Liquid. |
lv | Liquid to vapour phase change. |
LE | Leading edge. |
m | Molar. |
O | Initial |
o | Oil. |
p | Pool. |
s | Spilling liquid. |
v | Vapour. |
w | Water. |