ライフサイエンスコーパス: absolute temperature

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1 (where k is a Boltzman constant and I is the absolute temperature)).

2 (where k(B) is Boltzmann's constant and T is absolute temperature).

3 bit (kB is Boltzmann's constant and T is the absolute temperature).

4 temperature increase rather than just to the absolute temperature.

5 trical resistivity, thermal conductivity and absolute temperature.

6 , k(B) is Boltzmann's constant, and T is the absolute temperature.

7 the total thermal conductivity, and T is the absolute temperature.

8 ial's thermoelectric properties and T is the absolute temperature.

9 ere Ka is the affinity constant and T is the absolute temperature.

10 ent errors of less than four per cent of the absolute temperature.

11 to temperature synchronization at different absolute temperatures.

12 plots of logarithmic mobility vs reciprocal absolute temperature and compared for the linear and bra

13 (where k is a Boltzman constant and T is the absolute temperature)), and thiophosphorylation increase

14 At a given absolute temperature, as the sn-1 acyl length adjacent t

15 al increase in the rate upon increase of the absolute temperature by a factor of 2.

16 The pressure and absolute temperature dependences of transport properties

17 n sample concentration, ligand affinity, and absolute temperature; in most cases, the equilibration t

18 We finally suggest that the near absolute temperature-independence of 15N-KIE may point t

19 ccumulation of CBF transcripts, but instead, absolute temperature is monitored with a greater degree

20 T, where kB is Boltzmann's constant and T is absolute temperature (kelvin).

21 ty that is proportional to the square of the absolute temperature plus a term proportional to the squ

22 (DQC) points describes phase transitions at absolute temperature T = 0 outside the standard paradigm

23 dent on the cooling rate, dT/dt, whereas the absolute temperature T is of less importance.

24 At the same absolute temperature, the phosphatidylcholine (PC) serie

25 tween the tetanic tension and the reciprocal absolute temperature was sigmoidal with half-maximal ten

26 es and the plot of tension versus reciprocal absolute temperature was sigmoidal, with a half-maximal

27 ZT (where Z is the figure of merit and T is absolute temperature), which governs the Carnot efficien

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