We then introduce the characteristic length to scale the eigencompliances and compliance matrices to compare translational compliances with rotational ones.
We introduce the characteristic equation of the beam's deflection and, with employing the recently developed automatic Taylor expansion technique (ATET), present deflection solutions in terms of the loading parameters to the Euler Bernoulli boundary value problem.
Then we introduce the characteristic longitudinal velocity v c ∗, according to the following criterion.
In Section 3, we introduce the characteristic radius of fractal dust and derive the sublimation distance for that dust.
Next, we introduce the characteristic function (Delta(boldsymbol {omega, lambda})) which characterizes the eigenvalues of BVPs (2.1) and (2.6) as roots of (Delta(boldsymbol {omega, lambda})).
Now we may introduce the characteristic function (omega ( lambda )) as omega ( lambda ): = omega_{ - varepsilon} ( lambda ) = frac{1}{D_{1}} omega_{varepsilon} ( lambda ) = frac{1}{D_{1}D_{2}}omega_{ + varepsilon} ( lambda ).
We introduce the characteristic radius s of a dust particle, which is defined as (7 where ∫ dv means an integration over volume, is the distance from its center of mass, and ρi is its interior density.
