Deciphering the information available from a QSAR model needs the study of coefficients of these properties as they appear in the top equations.
The top three equations with one external parameter (equations [15] [17]) have a mean RMSD of 0.144 v.u., which indicates that although the presence of an external parameter removes some flexibility in the shape of the curve, it does not necessarily reduce the fit.
The side fired furnace equations are algebraic equations, the top fired furnace equations are two-point boundary value differential equations which are solved using the orthogonal collocation technique.
(Top) FLT in Equation 3; (bottom) FLT in Equation 6.
In the QSAR model, the following properties appear in the top-most equations: χ(3) cluster, κ(1), Wiener index, Coulson charge on N3, Electrostatic charge on C2, Dipole moment (x), Total dipole, Octupole moment and Total energy.
The top-two equations prescribe recognition dynamics on expected states of the world.
The observers' data can be fit with exponential functions of radius versus rotation speed (for observer 1, top curve, the equation of the fitted line is: y = 11.22*exp(−0.0033*x); and for observer 2, the equation is y = 8.33*exp(−0.0039*x)).
Each side, no doubt, believed it would come out on top of the equation.
