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The derived equations of motion are discretized through the Galerkin method.
The derived equations of motion are discretized by applying the Galerkin method.
These equations of motion are discretized by using the Galerkin method.
The equations of motion are discretized by using the assumed modes method with the static deflection of the beam.
The equations of motion are discretized by using the Galerkin method.
The equations of motion are discretized using finite differences and solved numerically.
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The motion is discretized by expansion in terms of the damped complex eigenfunctions.
The partial differential equation of motion is discretized using the Galerkin method and the final set of ordinary differential equations are integrated numerically using a pseudo-arclength continuation and collocation techniques and the Gear backward differentiation formula.
Similarly, the ATM motion was discretized into 4 increments to match pitching phases ABERMAX (maximum external rotation in 90° of abduction, early cocking), ABER90° (mid acceleration), ABER80° and ABER45° (ball release).
In finite element solution, the differential equation of motion is discretized into a number of finite element equations which form a system of algebraic equations to be solved: [K]{u} = {F}, where [K] is the stiffness matrix, {u} is the nodal displacement vector and {F} is the applied load vector.
The nonlinear governing equations of motion of plate are discretized in space and time domains using the discrete singular convolution and the differential quadrature methods, respectively.
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