Sentence examples for bond equilibrium from inspiring English sources

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For that specific case, the GNRs have one side fixed (1.598 nm for the armchair, and 1.349 nm for the zigzag), with minimized thickness d equal to 0.074 and 0.077 nm and C-C bond equilibrium lengths of l = 0.142 nm for the armchair and zigzag cases, respectively.

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Moreover, in previous work, we also showed that canonical synapse formation by purely passive mechanisms based on differences in the properties of the BCR/Ag and LFA-1/ICAM-1 bonds (e.g., equilibrium bond length, bond stiffness, affinity) is not possible, especially for high affinity antigens on a cell membrane that undergoes deformation.

A harmonic restraint was applied to backbone particles to mimic secondary structure stabilizing hydrogen bonds, with an equilibrium bond length of 0.6 nm and a force constant of 1000 kJ/mol/nm.

The first was to note that, for a linear hydrogen bond at equilibrium, the O−H and H···O bonds must exert equal and opposite forces on the H+ ion.

In finite size rectangular single layer graphene sheets (SLGS), the lengths of the C-C bonds at equilibrium after mechanical loading are unequal, ranging between 0.136 and 0.144 nm, and depend on the type of loading, size and boundary conditions [17, 18], as well as the location on the SLGS itself (i.e. the edges [19]).

Notably, in many water-addition reactions to carbon carbon double bonds, the equilibrium can be on the side of the starting material although the reaction is performed in water.

The expressions for the energies in eq 2 are as follows: (a) internal energy UINT where Kb and Kθ are the harmonic force constants, b0 and θ0 are the equilibrium bond length and bond angle, respectively, b and θ are the actual bond length and bond angle, respectively, Vn is an energy constant, n is the dihedral multiplicity, ø is the actual torsion angle, and δ is phase shift.

Bonds involving hydrogen were constrained to their equilibrium bond lengths using LINCS.

This is due to the longer C-Si equilibrium bond length compared to C-C bonds, which allows the Si-doped films to accommodate higher structural disorder.

The SHAKE algorithm was used to constrain all bonds containing hydrogen bonds to their equilibrium lengths.

Away from the equilibrium bond length, the SPF function underestimates and overestimates the Murrell Sorbie energy curve for bond compression and stretching, respectively, for most diatoms.

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