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The displacement of drops of KCl (100 mM) was carried out under a tension of 120 VDC.
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However, certain forces such as hysteresis or viscous forces can hinder the displacement of the drop.
Concretely, it is necessary that the driving force is higher than the force of hysteresis in order to obtain a displacement of the drop.
This state is problematic, in particular in microfluidic microsystems where the displacement of a drop with a hysteresis of 100° is not easily realizable.
Fig. 16 Load-displacement curves of drop-weight impact test and bottom-face damage patterns (experimental and numerical results) at specific points (Pascal et al. 2015).
Although the model is capable of fitting the pressure drop profiles during displacement of the MBL with water, the pressure drop calculated by the model is higher than that obtained experimentally during displacement of the MBL with the polymer solution in the channel bed.
The mismatch between the model and experimental pressure drops for displacement of the MBL with the polymer is explained in terms of the limitations of the model.
As shown, for vertical wells and horizontal wells, with the increase of displacement pressure-drop, the threshold temperature (or the certain-productivity temperature) shows a reducing trend.
An analytical expression of the important parameters including the maximum displacement, the maximum acceleration of dropping shock response and the dropping shock duration is obtained.
The displacement and acceleration response of dropping shock process by RHM are compared with those by the R-K method as shown in Figures 3 and 4, respectively.
The curve for the specimen dropped slightly at displacement of 293 mm when one of the tension re-bars fractured.
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