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Analytical integration results in equations for the stress strain curve, the hysteresis loop and the cyclic stress strain curve inherent to the model.
To this end we just varied the value of the θ XylR parameter in equations for Pu and Ps.
Although ƬE applies to the exhalation phase of breathing, it is a required mathematical term in equations for determining inspiratory Pplt, Crs, and Rtot.
Our approach simplifies these methods by using only the 0.10 to 0.50 seconds portion of the exhaled VT and flow rate curves to derive a slope for determination of ƬE, and then use ƬE in equations for determinations of Pplt, Crs, and Rtot.
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Now, making the change of variable and in equation for we obtain (2.87).
In linear approximation the slope in equation for foE dependence on F10.7 activity index may differ by ∼20% for summer and winter and for low and middle latitudes.
The dynamical equations are different from Tyson's model in two points: two new equations for Lox and miR369-3 and one additional term in equation for CycD to show the inactivation of CycD by Lox.
For example, the program now includes all five modular rate laws described in recent work in kinetic equations for large-scale kinetic modeling [ 35].
The corresponding differential equations have additional terms, similar to those in Equations 5– 8, for the new reactions.
First, we would like to explain our assumption in Equations (1- 3) for the removal due to the experimental samplings.
In Table 1, values in the equations for the proposed regression model were incorrect.
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CEO of Professional Science Editing for Scientists @ prosciediting.com