ライフサイエンスコーパス: measured value

1 ickness-dependent sensor admittance with the measured value.

2 is in very good agreement with the directly measured value.

3 rease of only 8% below that of the initially measured value.

4 give a binding energy in agreement with the measured value.

5 cted to within 0.25 MJ (60 kcal) of the mean measured value.

6 22)kcal/mol, in excellent agreement with the measured value.

7 bilayer agrees well with the experimentally measured value.

8 as within the 95% confidence interval of the measured value.

9 nificantly different from the experimentally measured value.

10 ly from In-Check tended to be lower than the measured value.

11 e at [C] = 0 is only 16-fold larger than the measured value.

12 lows us to obtain more accurate and reliable measured values.

13 and twist-stretch coupling in agreement with measured values.

14 of estimates at least 20% different from the measured values.

15 y of height estimates were within 10% of the measured values.

16 hniques generally showed good agreement with measured values.

17 f three different sizes agreed well with the measured values.

18 constants within the range of experimentally measured values.

19 ptides having a mass within 2 Daltons of the measured values.

20 index and grain yields all agreed well with measured values.

21 bility to within 5-10% of the experimentally measured values.

22 d 90Y-CC49 activity concentrations bracketed measured values.

23 V/K, which complicated interpretation of the measured values.

24 ed extinction coefficients within 20% of the measured values.

25 processing protocol parameters affected the measured values.

26 x, body height, age, and spinal level on the measured values.

27 h were in good agreement with experimentally measured values.

28 ed podocyte density estimation upon input of measured values.

29 vided predictions within approximately 3x of measured values.

30 filling Rsoil estimates of each technique to measured values.

31 uted from first principles, agrees well with measured values.

32 excellent agreement with the experimentally measured values.

33 30% for scattering coefficient with that of measured values.

34 sults in strong agreement with traditionally measured values.

35 rengths that are in very good agreement with measured values.

36 how significantly larger deviations from the measured values.

37 te costs based on both reported and neurally measured values.

38 variations in the varphi values are close to measured values.

39 e for removing the blank contribution to the measured values.

40 The measured value, 0.37+/-0.01 J m(-2) for the incommensura

41 The measured value, 0.84 +/- 0.06 eV, is higher than that pr

42 atch reasonably well with the experimentally measured values: 1.16 +/- 0.02 for the beta-linkage (com

43 excellent agreement with the experimentally measured value 10.1 +/- 0.8% for the octapeptide des-Arg

44 e methionine amino acid is very close to the measured value (14.7 +/- 1.2 versus 15.5 +/- 0.02 kcal/m

45 er than the computed value (25 muC/cm(2)) or measured value (55 muC/cm(2)) for the state-of-the-art o

46 dividual predicted values varied widely from measured values (95% limits of agreement, -460 to +424 k

47 dividual predicted values varied widely from measured values (95% limits of agreement, -632 to +573 k

48 tional diffusion coefficient is fixed at its measured value and alpha is eliminated in favor of P(d).

49 ifferences in energy expenditure between the measured value and the prediction estimated for some pat

50 A downward trend in the measured values and a shift towards soft tissue values w

51 as calculated on the basis of experimentally measured values and biokinetic data in humans.

52 de binding prediction, to the experimentally measured values and concluded that these are in good agr

53 , a linear correlation was found between the measured values and Hammett sigma constants.

54 as spheres, poor agreement was found between measured values and Stokes-Einstein predictions.

55 The average absolute difference between the measured values and the values predicted using these upd

56 es for both T(M) (within 10 degrees C of the measured value) and deltaGo(37) (within 0.8 kcal/mol of

57 ical predictions of the gill resistance with measured values, and provide a general model for examini

58 ransitions states, whose energies agree with measured values, and provide insight to the mechanism of

59 (13)C methyl residual dipolar couplings with measured values, and the level of agreement is at least

60 he fit model were compared to experimentally measured values, and we find that while some objectives

61 If measured values are absent, then empirical relationships

62 At low and intermediate resolutions, our measured values are considerably higher than obtained pr

63 Our measured values are consistent across the many different

64 Other possible contributions to the measured values are discussed.

65 The measured values are in good agreement with previous meas

66 extensive data sets based on experimentally measured values are not always available.

67 to be changed in a kinetic model if in vivo measured values are not reproduced.

68 F , and verify that the behaviours of these measured values are qualitatively different.

69 models were 0.22-0.25 units higher than the measured values (assuming all iron in the system was in

70 ry background Atlantic CO mixing ratios from measured values at Egham.

71 ts at low concentrations, but underestimated measured values at high concentrations.

72 at concentrations in general agreement with measured values at nearby monitoring sites.

73 We correlate these measured values, based on fluorescence microphotometry o

74 ed in an increase in PhiSO, with the highest measured value being 9.3%.

75 ll or quadrant RNFL thickness was defined by measured values below 5% of the norm.

76 ions calculated pK(a)s and E(m)s differ from measured values by less than 1 pH unit or 35 mV, respect

77 ar bead models of a triskelion show that the measured values can be accounted for by bending the legs

78 he Tanford-Wyman linkage relationship to the measured values demonstrates that the apparent pK(a) val

79 ions were found to be in good agreement with measured values, demonstrating the importance of the tai

80 ically significant correlation with directly measured values, estimation of systolic pulmonary artery

81 ies can be quantitatively evaluated from the measured values even for compounds without repeated unit

82 The measured value excludes a model within the tensor-vector

83 The measured value for Murchison is the largest enantiomeric

84 AM has been estimated to be -0.99 V from the measured value for S-3',4'-anhydroadenosyl-l-methionine.

85 This value is similar to the measured value for the critical monolayer tension of mem

86 a 65-kDa protein, which agreed well with the measured value for the purified enzyme.

87 the relative percent differences between the measured values for 100-200 duplicate samples, and throu

88 ted by this approach agreed fairly well with measured values for 11 different PNA:DNA duplexes, as we

89 The model provides good agreement with the measured values for both T(M) (within 10 degrees C of th

90 tion (126-160 kJ/mol) were within previously measured values for bulk Mg.

91 The measured values for Delta G(H*)* were all 57 kcal/mol, w

92 the model is consistent with experimentally measured values for electromechanical properties.

93 ally explained up to 22% of the variation in measured values for endogenous intestinal calcium.

94 within a few percentage points of published measured values for free-living Americans; the model, th

95 Measured values for glucose concentrations in phosphate-

96 We recorded some of the highest measured values for lateral and forward acceleration, de

97 predicted from PET data correlated well with measured values for Pa(O2) (r2= 0.91, p < 0.01) and Pa(C

98 or aerosol-water distribution underestimated measured values for PCBs by factors of 1-17 and for PCDD

99 argely fall within one standard deviation of measured values for perfluorinated alkyl acids (PFAAs).

100 Based on measured values for Stokes radius (29 A) and sedimentati

101 in agreement with previously calculated and measured values for stretching surface-tethered molecule

102 res are reproduced when using experimentally measured values for the CRU Ca2+ sensitivity (approximat

103 The measured values for the electric field gradient (EFG) or

104 Measured values for the reorganizational energy and hete

105 direct comparison between the calculated and measured values for the resonance wavelength shift of th

106 and deltaGo(37) (within 0.8 kcal/mol of the measured value) for hairpin formation.

107 changes were in agreement with independently measured values from isothermal titration calorimetry st

108 ring the estimated dimensions to empirically measured values from the original carcass.

109 The measured values, however, are close to PO2 estimates usi

110 n computed NC rupture-force distribution and measured values in atomic force microscopy (AFM) experim

111 a, and the time of the nadir corresponded to measured values in mice.

112 es that are in reasonable agreement with our measured values indicate that future total levels of (13

113 ssociation constants, K, agree well with the measured values: K is typically about 10-fold smaller th

114 FeMoco(resting), in good agreement with the measured value of -0.042 V in Azotobacter vinelandii; an

115 ent was generated, as verified by a negative measured value of -0.16 for the swap entanglement witnes

116 ll turgor pressure with a deviation from the measured value of 0.01 MPa.

117 t no detection of atmospheric methane with a measured value of 0.18 +/- 0.67 ppbv corresponding to an

118 cumulation was transient, reaching a maximal measured value of 1 micro M.

119 y from 99.5 (gas phase) to an experimentally measured value of 45.8 kilocalories per mole (agreeing c

120 that k(s) for FAD on CNTs is faster than the measured value of 7.6 s(-1).

121 microm is consistent with the experimentally measured value of 9.0 +/- 0.5 microm.

122 O2] <94%) or modified oximeters (displayed a measured value of 90% as 94%, therefore oxygen not given

123 light differences in nucleosome density, the measured value of f for both fragments was consistent wi

124 The measured value of f is consistent with a rod-like partic

125 er had a much greater effect, decreasing the measured value of k(f) by a factor of about 25 to 30, an

126 The measured value of sigma(2) can be significantly smaller

127 The mean measured value of tau was 30.5 d, with a range of 0-50 d

128 assume charge superposition and use the best measured value of the antiproton charge, then we can pla

129 Our measured value of the appropriate Bell's 'signal' is 2.2

130 he outer segment can readily account for the measured value of the axial diffusion coefficient, as th

131 nts at I = 0.1 mM, consistent with the lower measured value of the diffusion coefficients at this ion

132 on of estimated energy requirements with the measured value of total energy expenditure (TEE) from DL

133 The measured values of (237)Np and (239)Pu by AMS exhibit go

134 a produced a correlation between modeled and measured values of 0.70 for B73 and 0.69 for br2.

135 e in excellent agreement with experimentally measured values of 12 kcal/mol and 5 ms, respectively.

136 ed in resting and growing NIH3T3 cells, with measured values of 30-35 and 70 min, respectively.

137 o, and MoFe:Fe protein ratio, in contrast to measured values of 4.0-25 when DT is used under the same

138 2) plane possesses the highest hardness with measured values of 40.5 and 36.4 GPa, respectively.

139 contributions to the value of a by comparing measured values of a for DNA containing a generic sequen

140 Measured values of both chi(0) [(12.4 +/- 2.0) x 10(-4)

141 Measured values of cardiac output and stroke volume are

142 he nucleus, we could accordingly correct the measured values of cell Cl-.

143 analyze profiles of concentration fronts and measured values of D for phenylalanine to within 5% of p

144 The measured values of delta15N have an average analytical p

145 We conclude that the experimentally measured values of DeltaC(p,obs) for SSB binding to ssDN

146 ed in establishing a concordance between the measured values of Em and those calculated from the corr

147 o bend or tilt, but depend critically on the measured values of filament sliding and elastic strain.

148 is no known model capable of predicting the measured values of gamma nor its variation among differe

149 ound to be insufficient to explain the lower measured values of glyoxal relative to other biomass bur

150 However, measured values of H+/La3+ exchange indicate that only 4

151 The measured values of intrinsic viscosity agree remarkably

152 Comparison of the measured values of k(1d)/k(1e) and k(1f)/k(1g) is theref

153 ative stiffness of naked DNA is evident from measured values of longitudinal persistence length (appr

154 ilar to thetaf observed for comet nuclei and measured values of other rigid aggregated systems across

155 amel and dentin specimens and to compare the measured values of reflectance with K-M theoretical valu

156 The model reproduces experimentally measured values of ring tension, explains why nodes move

157 y losses were 11-65% greater than when using measured values of Rlight .

158 The measured values of S, from numerical fits of magnetizati

159 The model agrees well with measured values of swimming speeds during steady state a

160 ed by conventional methods, we show that the measured values of the bubble conductance with known bub

161 osmotic pressure differences associated with measured values of the critical concentration of incubat

162 Finally, it is shown that the measured values of the glucose, urea and creatinine conc

163 Based on measured values of the heat capacity, radius of gyration

164 Upon introducing measured values of the model parameters for Band 3 in er

165 t between model-predicted and experimentally measured values of the rates of oxygen and glucose consu

166 nd leads to accurate approximations in which measured values of the surface intensity are shown to be

167 Our model recovers the experimentally measured values of the tension in fish keratocytes and t

168 ressures (Pmci,c, Pmcd,c, and Pinf,c) to the measured values of the total respiratory system.

169 egrees C determined from the experimentially measured values of the transition enthalpy, DeltaH(cal),

170 The measured values of whole blood from the micro-channel (4

171 ffects of Trolox and bound antioxidants with measured values on lipid oxidation revealed synergetic i

172 sed V(A)/Q distributions closely agreed with measured values (partial pressure of oxygen, arterial [P

173 bution, and those values are compared to the measured values presented here.

174 The conversion of a measured value Q(exp) of an observable quantity Q into s

175 ual LCs, which agreed well with the actually measured values (r = 0.96, P < 0.001).

176 ltagtr values show a strong correlation with measured values (R = 0.99).

177 tion forecasts significantly correlated with measured values (r(2) = 0.67; P < 0.001).

178 lectrode immersed in blood serum because the measured value reflects the state of equilibrium between

179 have also been calculated and compared with measured values, showing both spatial and temporal varia

180 coefficients (Gamma(23)) and experimentally measured values suggests that semiquantitative agreement

181 ature, and were quantitatively closer to the measured values than those derived from the intuitive, a

182 ters, were in much better agreement with the measured values than were predictions based on other app

183 ement modeling suggested a correction to the measured values that brought the transition temperatures

184 We call these measured values the momentums of the published statement

185 e in excellent agreement with experimentally measured values, this method does not scale up, and is l

186 ween the nominal values of standards and the measured values varied, depending upon the assay used an

187 The measured value was G = (6.6873 +/- 0.0094) x 10(-11) m3

188 but when combined with crankcase emissions, measured values were 11.4% lower than predicted by AP-42

189 Correlations between measured values were assessed by means of Pearson correl

190 Measured values were compared with those reported in lit

191 Measured values were used to derive a predictive equatio

192 e shear modulus predicted corresponds to the measured value when the interparticle adhesive energy is

193 trations were within a factor of 2 to 9 from measured values, while air concentrations back-calculate

194 The technique was evaluated by comparing measured values with a range of isotopically enriched su

195 en performed to establish the association of measured values with potential predictors.

196 The measured values with the Bi-FE were in good agreement wi

197 designed for this purpose, and compared the measured values with these tissues' mutual spreading beh

198 ICE models (>90%) were within 5-fold of the measured values, with no influence of taxonomic relatedn