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the contact angle
As the DHPDMS content increases above 5%, both the contact angle and the surface tension tend to approach a constant.
      
The contact angle increases with increasing temperature, and it tends to approach a constant when the temperature is higher than 50°C.
      
Based on the contact angle data, the surface energy was obtained from the acid-base approach.
      
The results obtained cannot be explained in terms of hydrodynamic and barrier theories of the contact angle.
      
The contact angles are shown to increase with a decreasing microsphere radius, whereas the hysteresis of the contact angle decreases.
      
It was also established that, for the investigated systems, the contact angle is virtually independent of the composition of the liquid phase.
      
The contact angle in saturated water vapors, θv = 84°, was calculated from these values.
      
After adsorption, the quartz surface is hydrophobized: the contact angle measured by the bubble method is close to 33°-34°.
      
For alkanes and water, and in a limited range of drop sizes where gravity can be ignored, the model accounts very well for the dynamics of the drop radius, and rather well for the contact angle.
      
It is shown that for individual classes of natural media the residual gas saturation depends only on the porosity and the contact angle of wetting.
      
The Hocking condition is used to take into account the contact angle dynamics.
      
The Hocking condition is used to take into account the contact angle dynamics.
      
The charge density created under different treatment conditions was correlated with the contact angle.
      
The dependence of the contact angle on the discharge current and treatment time was examined.
      
The surface-charge density was correlated with the contact angle for various treatment conditions.
      
The contact angle for water changed from 75° to zero.
      
The contact angle on the silaned glass plates reaches 125°.
      
At bending glass plates, the contact angle is always larger on the convex (stretched) side than on the concave (compressed) side.
      
The contact angle velocity is found (this angle determines the meniscus boundary).
      
Formulas relating the distribution characteristics to the contact angle and the curvature radius of the liquid surface are derived and experimentally verified.
      
 

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