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1 (where k is a Boltzman constant and I is the absolute temperature)).
2 bit (kB is Boltzmann's constant and T is the absolute temperature).
3 (where k(B) is Boltzmann's constant and T is absolute temperature).
4 temperature increase rather than just to the absolute temperature.
5 the total thermal conductivity, and T is the absolute temperature.
6 ent errors of less than four per cent of the absolute temperature.
7 trical resistivity, thermal conductivity and absolute temperature.
8 , k(B) is Boltzmann's constant, and T is the absolute temperature.
9 exhibiting sustained firing that scales with absolute temperature.
10 ial's thermoelectric properties and T is the absolute temperature.
11 ere Ka is the affinity constant and T is the absolute temperature.
12 ection of change (heating or cooling) and of absolute temperature.
13  to temperature synchronization at different absolute temperatures.
14 worsening heat, above and beyond that of the absolute temperatures.
15 ate configurations characterized by negative absolute temperatures.
16 econciled by linearization of the inverse of absolute temperature (1/T) and heating temperature (T),
17 warming is not only unparalleled in terms of absolute temperatures(5), but also unprecedented in spat
18  plots of logarithmic mobility vs reciprocal absolute temperature and compared for the linear and bra
19 d shared ON- and OFF-type representations of absolute temperature and rates of change.
20 in-insensitive intrinsic variable to measure absolute temperature and the normalized capacitance as a
21 (where k is a Boltzman constant and T is the absolute temperature)), and thiophosphorylation increase
22        Cumulative marine heatwave intensity, absolute temperature, and location within a species' ran
23 ons we show that, despite large increases in absolute temperature, anomalies relative to our empirica
24                                   At a given absolute temperature, as the sn-1 acyl length adjacent t
25 ontinuous increase of the direct effect with absolute temperature, but is it observed experimentally?
26 hibit sustained firing rates that scale with absolute temperature-but only for temperatures above the
27 al increase in the rate upon increase of the absolute temperature by a factor of 2.
28                             The pressure and absolute temperature dependences of transport properties
29 in fatty tissue and requires a reference for absolute temperature determination.
30 t ~3 degrees C warming across the MECO, with absolute temperatures generally in accordance with trace
31  resistivity measured in mOmega cm, T is the absolute temperature in K, S is the Seebeck coefficient,
32 n sample concentration, ligand affinity, and absolute temperature; in most cases, the equilibration t
33                               Contrastingly, absolute temperature increase has a negligible associati
34                                      Maximum absolute temperature increase recorded along a complete
35 urface temperature (SST) extremes as well as absolute temperature increase.
36             We finally suggest that the near absolute temperature-independence of 15N-KIE may point t
37 ervous system selectively encodes and relays absolute temperature information and illustrate a sensor
38 ccumulation of CBF transcripts, but instead, absolute temperature is monitored with a greater degree
39 T, where kB is Boltzmann's constant and T is absolute temperature (kelvin).
40 n intensive care 21-fold (P = 0.016), whilst absolute temperature maxima or minima did not predict ou
41 s such as the fruit fly Drosophila depend on absolute temperature measurements to identify external c
42       This device can be used to measure the absolute temperature of an object by comparing the relat
43 ty that is proportional to the square of the absolute temperature plus a term proportional to the squ
44  (DQC) points describes phase transitions at absolute temperature T = 0 outside the standard paradigm
45 dent on the cooling rate, dT/dt, whereas the absolute temperature T is of less importance.
46     The reaction rate k as a function of the absolute temperature T is then determined by diffusion o
47 lack body increases with the fourth power of absolute temperature (T(4) ), an effect known as the Ste
48                                  At the same absolute temperature, the phosphatidylcholine (PC) serie
49 etations to achieve both reliable trends and absolute temperature values, while providing a more opti
50 tween the tetanic tension and the reciprocal absolute temperature was sigmoidal with half-maximal ten
51 es and the plot of tension versus reciprocal absolute temperature was sigmoidal, with a half-maximal
52  ZT (where Z is the figure of merit and T is absolute temperature), which governs the Carnot efficien