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In "Discussion" section, we discuss the breaking points of the double power-law-type spectrum by examining the dependence of the break point energy on other parameters.
We discussed the dependence of the break point, (p_b), on other shock parameters, and showed that the value of (p_b) can be estimated by balancing the convection and diffusion in a region between the two shocks.
There is no clear way to directly compute Pr BT [i,1] = 1) since we do not know all the determinants of a break and the precise dependence of the break probability on those determinants.
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The elasticity of π C ∗ to all joined wood densities was 1 (Figure 3A), evidencing a proportionality dependence of the break-even carbon price on this parameter.
Figure 3 shows the β⊥i dependence of the measured break frequency normalized to the frequencies corresponding to the ion gyroscale and ion inertial length, = vsw/(2 π ρi) and = vsw/(2 π di), where vsw is the solar wind speed.
The dependence of the passivation potential or the break potential from the chromium concentration in the alloys and the water concentration in the solution has been determined.
In this section, we discuss the dependence of spectrum breaking using Eqs.
Some synergism has been observed in the PE/SBR composition dependence of the tensile strengths at yield and break.
The feed composition dependence of the LLX minimal heat duty can result in a feed compositional break-even point when comparing LLX with ED.
When the two oscillators are anharmonic, the amplitude dependence of their frequencies breaks, in general, any eventual initial resonance so that no substantial energy transfer occurs unless, exceptionally, an almost perfect resonance persists.
Once the symmetry of the thermodynamic driving force has been broken, the kinetics lead to further asymmetry due to the force dependence of the unbinding rate.
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