Sentence examples for equilibrium above from inspiring English sources

For all catalysts studied, the reaction attained almost equilibrium above 500 °C at the space velocity of 20,000 l kg−1 h−1.

Conforming with the existing literature, we find that the reduction of habitat size, or increasing of species movement rates equivalently, has the potential to decrease the amplitude of oscillations and even bring the system to a steady coexistence equilibrium above a threshold.

Nevertheless, Lonker et al. (1993) identified some departures from equilibrium above 200 °C, which he attributed to some kinetic effects.

In JWBG2 the existence of cycles in equilibrium above this line is not confirmed, while in JWBG1 their existence is established for (c<1), and their necessity is proved for (c>1) (Sect. 5.3).

In the light of the discussion of the equilibrium above, exactly one of these gives a positive solution for x0 and x1 under realistic parameter choices.

The time to converge on the quasi-equilibrium from above is especially prolonged in populations of large size because of the progressively reduced rate of production of antimutators as the population approaches a lower and lower mutation rate state.

An equivalent way of stating the above "equilibrium condition" is to write Y = C + I.

To alter the above equilibrium, type V AC was overexpressed in a myocyte-specific manner in the hearts of transgenic mice using the alpha-myosin heavy chain promoter.

For example, at a pH of less than 8, the principal reactions and their relative speed are as follows:CO2 + H2O ⇌ H2CO3 (slow) H2CO3 + OH− ⇌ HCO3− + H2O (fast) Above pH 10 the following reactions are important:CO2 + OH− ⇌ HCO3− (slow) HCO3− + OH− ⇌ CO32− + H2O (fast) Between pH values of 8 and 10, all the above equilibrium reactions are significant.

From satisfying the above equilibrium equations, one gets C2 = √2A2 = (2α π A1 - β C1) / (3 4 ν).

The equilibrium of the above difference equation is asymptotically stable since the roots of its characteristic polynomial are μ 1 = μ 2 = 0 and μ 3 = a.