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The lower plate is hydraulically shifted and is usually replaced after every heat.
The flow is induced by variable acceleration of the lower plate.
Using Equation 4, the shorter retention time of peak, the lower plate number is worked out.
The flow is induced by a linear acceleration of the lower plate in its own plane.
Lower plate angles resulted in lower liquid-side mass transfer coefficients.
They form, like the Iberia Newfoundland rifted margins, conjugate upper and lower plate margin.
An optimum design of a triangular cell along the lower plate is also presented.
In the SFTR, shear strain was given from the lower plate.
Plywood strips were kept on the lower plate of the testing device and specimens were placed on the plywood strip.
Similarly, the stress applied on the lower plate at any point ( x, y, − h ) can be calculated.
Gelled samples were placed on the lower plate, and the upper spindle was brought slowly to the 0.2-mm gap.
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