1. 실험목적
1. 측벽에 의한 유속의 변화
2. 수심에 따른 유속의 변화
3. 자유표면의 유속의 변화
2. 실험이론
2.1 유체(Fluid)
고체는 정적인 변형의 의해 전단응력에 저항 할 수 있으나 유체는 그러하지 못하다. 유체는 그것에 작용되는 전단응력이 아무리 작다고 하여도 운동을 시작한다. 유체는 전단
flow in a pipe or a sphere moving in a fluid the internal diameter is generally used today. Other shapes (such as rectangular pipes or non-spherical objects) have an equivalent diameter defined. For fluids of variable density (e.g. compressible gases) or variable viscosity (non-Newtonian fluids) special rules apply. The velocity may also be a matter of convention in some circumstances, notably st
surface, improved solubility, targeted drug delivery and multifunctionality, nanoparticles have emerged as potential drug delivery carriers to tissues throughout the body. Yet passing the BBB is particularly difficult. The proper design of such engineered ‘nanocarriers’ becomes very important in transversing the impermeable membranes to facilitate drug delivery. At the same time, it is also r
-surface triangle: 메쉬의 개수를 나타낸다.
-connectivity regions '1' : 모델 전체가 하나로 연결되어 있다는 것을 의미한다.
-free edges '0' : Fusion 모델은 반드시 free edge 값이 0이어야 한다.
-non-mainfold edges '0' : Fusion 모델은 반드시 non-mainfold 의 개수가 0이어야 한다.
-element not oriented '0' : Fusion 모델은 반드시 0이어
surface morphology and roughness of the films was observed by field emission scanning electron microscopy (FE-SEM, Model: JSM-6701F) and atomic force microscopy (AFM, Digital Instrument, nanoscope III) operated at room temperature, respectively. The electrical properties of the films were determined using Hall measurement system (Van der Pauwconfiguration, Hilton, Australia) at room temperature.