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This coefficient is found to be dependent on the collision velocity, but becomes constant for strong collisions.
Note that the PoD for RADOI becomes constant for SNR ≤ 3 dB, which corresponds to a biased estimation.
Consequently, the sequence ({ z_{n} } ) in both cases becomes constant for (ngeq n_{0}) and hence (2.2) holds.
Consequently, the sequence ({z_{k}}) becomes constant for (kgeq k_{0}) and (z_{k_{0}}) is a coincidence point of the pairs ((f,S)) and ((g,R)).
When the failure limit is reached, then the strain energy becomes constant for the rest of the deformation process precluding the material healing.
Consequently, the sequence ({d_{k}}) becomes constant for (kgeq k_{0}) and hence (lim_{krightarrowinfty} d(x_{k},x_{k+1}) = 0).
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For a given pressure above the LPDL, burning rates eventually became constant for both increasing and decreasing particle sizes.
The TEC values almost become constant for F10.7 values in the range of 200 to 300.
The amplitude ratio | Z 1 | Open image in new window sharply decreases to become constant for MIT, while for the case of MTIT, its value sharply increases then sharply decrease to become constant at the end.
The static shear strength becomes constant after LFC for D r = 60% as well as for D r = 78%, though dry density decreases and permeability remain constant.
The static shear strength becomes constant after LFC for D r = 60 and 78%.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com