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In the hard sciences, when dealing with complex systems people have often used higher-level, aggregative concepts that seem to work empirically long before they have a full derivation of effects from the underlying laws of physics.
A full derivation of how RSL is determined is beyond the scope of this article.
In Appendix A we give a full derivation of this expression.
A full derivation of this equation and that for the post-SN eccentricity is given in Appendix A.1.
In this paper a full derivation of the multiphase fluid flow equations in a poroelastic environment is presented to accurately reflect the fluid flow behavior and evaluate fluid recovery under different driving mechanisms.
A full derivation of the change in semi-major axis (Eq. (33)) and eccentricity (Eq. (78)) of the outer orbit due to a SN in the inner orbit, are given in Appendix A.1.
Similar(52)
From a steady-state assumption (d x/d t = d y/d t = 0), we have the following equation: 2where X and Y are the experimentally observed fluorescence data for DsRedE and L7Ae-ECFP; κ is a pseudo dissociation constant; and γ is a constant (see Supporting Information for the full derivation and explanation).
We now observe that the reduced model has two distinct behaviours depending on whether the dynamics are occurring in a saturated or non-saturated state (for full derivation, see Additional file 1).
If so, we derived the final prediction model from the full derivation sample [ 19].
Here we present its full derivation, provide more details and examples, include introductions from an animal reservoir and show how the method can be used to provide statistical expectations for new case predictions.
The full derivation with assumptions are presented.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com