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991.
992.
993.
单相旋转型驻波超声电机的数学模型及仿真 总被引:1,自引:0,他引:1
尽管单相驱动的旋转型驻波超声电机的原理样机早巳研制成功,但对这类电机的运动机理的研究却一直局限在定性分析上。本文将从能量角度,根据Hamilton变分原理,定、转子摩擦界面采用纯滑动模型建立了该种电机的数学模型;并根据此模型,用MATLAB语言作了计算机仿真,得到了该种电机的开、关过程动态响应。 相似文献
994.
MIMU/GPS组合导航系统研究 总被引:4,自引:0,他引:4
根据智能交通对车辆导航和定位的要求,研究了MIMU与GPS松散组合导航系统,以速度、位置作为观测量设计了Kalman滤波器。为了验证系统的性能,利用MIMU实验室测试数据和GPS仿真数据对该组合导航系统进行了半物理仿真,分别给出了纯MIMU、组合导航系统及GPS信号短时间丢失时的位置误差仿真曲线。分析结果表明组合系统具有良好的长期工作精度,能够满足车辆导航和定位的要求。 相似文献
995.
各向异性本构关系在板料成形数值模拟中的应用 总被引:7,自引:0,他引:7
对几种能表达面内各向异性的屈服准则Hill、Barlat-Lian、Barlat进行了比较。以弹性变形服从各向同性广义虎克定律的情况下,给出了基于张量算法推导的弹塑性本构关系的一般表达式,并由此导出了相应屈服准则的弹塑性本构关系的显式表达。借助ABAQUS软件本构模块用户子程序接口,分别实现了这些屈服准则在ABAQUS的嵌入。以模拟方形盒的拉延过程为例,分析了不同的屈服准则在板料成形过程数值模拟中的应用。模拟结果表明,基于弹塑性本构关系一般表达所列出的相应屈服准则的显式表达式是正确的;在采用壳元来模拟板料成形时,采用Barlat准则的模拟结果和采用Barlat-Lian准则的结果差别不大。 相似文献
996.
本文用有限元方法分析了两种常见汽轮发电机定子结构模型的动力特性,建立了固有特性对集中质量、连接刚度及基础刚度的灵敏度分析方法,对这两种结构模型进行了振动实验研究,实验结果与有限元分析结果吻合较好.从避开共振的角度出发,对两种结构作了评价.本文的研究方法及实验结果对汽轮发电机结构设计、减振、隔振和降噪等方面的工作具有一定的参考价值和实际工程意义. 相似文献
997.
In a WAG process (Water Alternate Gas), water and a miscible solvent (gas) are injected into a reservoir containing water and oil. The solvent will finger through the oil, leading to early breakthrough and poor recovery. Compared with a miscible flood, when only solvent is injected, fingering is supressed by the simultaneous injection of water, since this reduces the apparent mobility contrast between the injected and displaced fluids. The fingering in a miscible flood, with only hydrocarbon flowing, can be modelled successfully using a Todd and Longstaff fractional flow. In this paper, we demonstrate how to modify the effective Todd and Longstaff mobility ratio self-consistently to account for fingering in three component systems. The resultant empirical equations of flow are solved exactly in one dimension and are in excellent agreement with the averaged saturation and concentration profiles computed using two dimensional high resolution simulation, for a variety of injected water saturations, in both secondary and tertiary displacements. 相似文献
998.
The behavior of a terminally anchored freely-jointed bead-rod chain, subjected to solvent shear flow, was investigated via Brownian dynamics simulations. Previous calculations have been improved by computing the segment density and fluid velocity profiles self-consistently. The segment density distributions, components of the radius of gyration, and chain attachment shear and normal stresses were found to be sensitive to low values of shear rate. Additionally, it was found that the thickness of a model polymer layer was a strong function of the shear rate, and that the functional dependence on shear rate changed dramatically as the chain length increased. For the longest chains studied, the thickness of the model polymer layer first increased as the shear rate increased, passed through a maximum, and then decreased at high shear rates, in accordance with experimental results in theta solvents. These results suggest that a dilute or semi-dilute layer model may explain hydrodynamic behavior previously thought to be due to the entanglements that occur in dense surface bound polymer layers.Nomenclature
a
i
acceleration of bead i
-
b
radius of the beads
-
d
length of the rods connecting the chain beads
-
d
i
vector from bead i to bead i + 1
-
F
i
external force applied to bead i
-
F
i
b
external force on bead i due to Brownian motion of surrounding fluid
-
F
i
h
external force on bead i due to viscous drag
-
F
i
s
external force on bead i due to surface interactions
-
f
Stokes drag coefficient
-
Boltzmann's constant
-
L
h
effective hydrodynamic thickness
-
m
i
mass of bead i
-
N
number of beads on a model chain
-
n
number of chains anchored to the surface per unit surface area
-
P
segment density distribution P pressure
-
Q
flow in a tube with no surface bound polymer layer
-
Q
a
flow in a tube with a surface bound polymer layer
-
R
g
vector representation of the radius of gyration
-
R
tube radius
-
r
radial coordinate in the tube geometry
-
S
ij
pair hydrodynamic interaction tensor for beads i and j
-
T
i
internal chain force in rod i connecting beads i and i + 1
-
T
X
component of the surface attachment force in the direction of the fluid flow
-
T
y
component of the surface attachment force perpendicular to the surface
-
T
temperature
-
v
i
velocity of the center of mass of bead i
-
V
if
average fluid velocity at the location of bead i
-
v
if
0
fluid velocity in the absence of a polymer chain
-
v
if
perturbation to the fluid velocity due to hydrodynamic interactions
-
V
b
bead volume = 4 b
3/3
-
scalar fluid speed in the axial direction down the tube
-
x
axial coordinate in the tube geometry
Greek symbols w
apparent shear rate
-
fluid viscosity
-
polymer layer permeability
-
volume fraction of space occupied by chain beads
- (w)a
chain attachment stress perpendicular to the surface
- (w)a
chain attachment stress in the plane of the surface and in the direction of fluid flow 相似文献
999.
1000.