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The proposed methodology is based on the minimum potential energy theorem written regarding nodal positions.
The governing equations and boundary conditions are derived using the minimum potential energy principle.
The equilibrium equations and boundary conditions are obtained by using the minimum potential energy principle.
The explicit solutions of bending deflection are determined using the minimum potential energy principle.
The twist response is bistable, and represents the minimum potential energy paths that join two orthogonally-oriented bending modes.
The system tends to have the minimum potential energy when the droplet moves to the softer end of the beam.
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In each case, the observed change in the minimum potentials, at an equilibrium distance of 0.3 nm, is shown in the left part of the figure.
The location of CO2 does not coincide as perfectly with the potential well as that of DME, but CO2 is along the linear minimum potential path, with the O atom on the potential minimum side.
Based on the theoretical model, the energy landscape for different buckling modes of SiNW on PDMS substrate is given, which shows that both the in-plane and out-of-plane buckling modes have the local minimum potential energy, whereas the helical buckling model has the global minimum potential energy.
For simplicity reasons, only the structure with the global minimum potential energy OPLS_2005 was retained and used as a template in the shape screening step.
For England, the maximum (minimum) potential area of SRC that would be grown on dairy, LFA grazing livestock and lowland grazing livestock farms is 54,603 ha (17,156 ha); the respective results for miscanthus are 43,859 ha (12,321 ha).
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