Example sentences of "[prep] t c " in BNC.

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1 ( In the extreme classical savings model , with , there is no way in which debt policy can be used to offset the effect of T c . )
2 The effect of the tax may be explored more fully by using the steady-state condition : ( 8–46 ) where w is a function of k and r is a function of t c and k .
3 Remembering that , where M and are the molar mass and partial specific volume of the polymer , and V 1 is the molar volume of the solvent , the equation states that the critical temperature is a function of M and the value of T c at infinite M is the theta temperature for the system .
4 The same is true for other temperatures lying below T c , and the inflexion points can be joined to bound an area representing the heterogeneous two phase system , where there is limited solubility of component 2 in 1 and vice-versa .
5 It 's er partly chlorine yes but it there are occasions when it smells like T C P .
6 In addition to probing the critical state near T c , these measurements allow the indirect determination of the residual , normal-state resistivity .
7 Figure 1a and b also shows ( T ) for K 3 C 60 and Rb 3 C 60 in greater detail near T c ( the temperature scale has been normalized to T c in each case ) .
8 In an earlier investigation of the resistivity of K 3 C 60 , fluctuation effects near T c were not resolved because of large scatter in the data .
9 But as shown in Fig. 1 a , the difference between the two extrapolations is small in the relevant temperature range near T c , and both are consistent with measured near T c at high magnetic field ( also shown in Fig. 1 a ) .
10 But as shown in Fig. 1 a , the difference between the two extrapolations is small in the relevant temperature range near T c , and both are consistent with measured near T c at high magnetic field ( also shown in Fig. 1 a ) .
11 Just above T c , thermodynamic fluctuations produce small , transient regions of the superconducting state , giving rise to an anomalous increase in the normal-state conductivity known as paraconductivity .
12 Just above T c , the resistivity for both materials deviates from its normal-state behaviour before dropping precipitously at T c .
13 For conventional 3-D superconductors , the fractional change in normal conductivity , too small to be observable in any meaningful temperature interval above T c .
14 On the other hand , with T c = 0 , the underlined term in ( 8–60 ) becomes .
15 Gargling with T C P .
16 Figure 1a and b also shows ( T ) for K 3 C 60 and Rb 3 C 60 in greater detail near T c ( the temperature scale has been normalized to T c in each case ) .
17 The impact on the steady-state growth path , assuming one exists , may be seen by differentiating the condition with respect to t c : where .
18 and s t denotes the derivative with respect to t c Where the steady-state path is locally stable , the coefficient of is negative , and k rises ( falls ) if s t is positive ( negative ) — as indicated by Fig. 8–2 .
19 Well we should use X-networking standards , and at the moment if a network complies to T C P I P as the communications protocol then we can work with that .
20 Just above T c , the resistivity for both materials deviates from its normal-state behaviour before dropping precipitously at T c .
21 As the temperature is increased the limits of this two phase co-existence contract , until eventually they coalesce to produce a homogeneous , one phase , mixture at T c , the critical solution temperature .
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