ライフサイエンスコーパス: measured value

1 nd 0.89, respectively, between predicted and measured values).

2 ickness-dependent sensor admittance with the measured value.

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

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

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

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

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

8 bilayer agrees well with the experimentally measured value.

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

10 nificantly different from the experimentally measured value.

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

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

13 actor binding sites to within 1 kBT of their measured values.

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

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

16 profiles of SVOCs and compared them with the measured values.

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

18 conditions can give rise to widely divergent measured values.

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

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

21 uniformity which was broadly consistent with measured values.

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

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

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

25 constants within the range of experimentally measured values.

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

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

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

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

30 the proportion of predictions within 10% of measured values.

31 excellent agreement with the experimentally measured values.

32 d-calculated volume achieved slightly higher measured values.

33 hite sturgeon within 1 order of magnitude of measured values.

34 a tendency existed toward overestimation of measured values.

35 ermined and the unknown uncertainty of their measured values.

36 d uniformity difference between designed and measured values.

37 tor which is in good agreement with directly measured values.

38 hniques generally showed good agreement with measured values.

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

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

41 d agreement the difference in experimentally measured values.

42 processing protocol parameters affected the measured values.

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

44 h were in good agreement with experimentally measured values.

45 ed podocyte density estimation upon input of measured values.

46 vided predictions within approximately 3x of measured values.

47 filling Rsoil estimates of each technique to measured values.

48 a and evaluate the impact of model choice on measured values.

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

50 30% for scattering coefficient with that of measured values.

51 ns corroborate the order of magnitude of the measured values.

52 sults in strong agreement with traditionally measured values.

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

54 how significantly larger deviations from the measured values.

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

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

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

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

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

60 dimerization (59 kJ mol(-1)) are similar to measured values (46 +/- 5 kJ mol(-1)) and the weak bindi

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

62 he predicted distributions did not cover the measured values (75% for liver, 90% for skeleton, and 50

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

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

65 h predicted energy expenditure within 10% of measured values ("accuracy").

66 he field uniformity between the designed and measured values after being constructed and charged, i.e

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

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

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

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

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

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

73 correlation analyses were conducted for the measured values and neurodevelopmental outcome scores.

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

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

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

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

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

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

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

81 If measured values are absent, then empirical relationships

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

83 Our measured values are consistent across the many different

84 Other possible contributions to the measured values are discussed.

85 The measured values are in good agreement with previous meas

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

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

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

89 sed-phase at the source, indicating that the measured values are reflecting the plume continuous-phas

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

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

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

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

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

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

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

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

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

99 e widely used, but the accuracy of these and measured values can be difficult to ascertain.

100 (diabetes mellitus and BP) by adjusting for measured values (conventional analyses) or genetic assoc

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

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

103 onstrate how uncertainties in experimentally measured values determine the uncertainty in P(EB).

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

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

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

107 The measured value for Murchison is the largest enantiomeric

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

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

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

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

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

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

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

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

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

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

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

119 oth amylose and amylopectin components, with measured values for gelatinization enthalpy and viscosit

120 Measured values for glucose concentrations in phosphate-

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

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

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

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

125 as observed between NIR-predicted values and measured values for PG, VG and nicotine (all R(2) > 0.95

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

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

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

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

130 Measured values for the reorganizational energy and hete

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

132 lower states in addition to providing newly measured values for the upper levels.

133 as less consistency between predicted and GC measured values for water due to the relatively high lim

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

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

136 n in the difference between the tumor volume measured values from the magnetic resonance imaging (MRI

137 es were in most of the cases higher than the measured values from the MRI.

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

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

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

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

142 the accuracy of predictive equations against measured values in posttreatment colorectal cancer survi

143 is two to three times larger than previously measured values in the first Landau level.

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

145 The measured value is always bipolar since the electric meas

146 ed carbamic acid acidities K(5) based on the measured value K(6) of aminocarbamic acid using isodesmi

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

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

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

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

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

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

153 02 +/- 9 Ma, corresponding to the physically measured value of 103 +/- 5 Myr, rather than the latest

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

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

156 The measured value of 700 mV, far exceeding the thermodynami

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

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

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

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

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

162 The measured value of responses at the optimized process con

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

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

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

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

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

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

169 Here we report the measured value of the EA of astatine to be 2.41578(7) eV

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

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

172 tosynthesis model is informed by local field-measured values of (a) fractional absorbed photosyntheti

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

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

175 l sequence dependence accurately predict the measured values of 271 helices in an updated database wi

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

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

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

179 This is above the measured values of [Formula: see text] and [Formula: see

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

181 macular volume (CMV) were measured; then the measured values of affected and fellow unaffected eye we

182 tical studies that use predicted rather than measured values of body composition.

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

184 Measured values of cardiac output and stroke volume are

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

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

187 The measured values of delta15N have an average analytical p

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

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

190 els reflect the corresponding experimentally measured values of epidermal and stratum corneum thickne

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

192 text] GHz which simultaneously improves the measured values of gain to 11.65 dBi, H-plane SLL to [Fo

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

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

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

196 The measured values of intrinsic viscosity agree remarkably

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

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

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

200 using the derived set of equations based on measured values of real (R) and imaginary part (X) of bi

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

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

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

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

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

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

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

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

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

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

211 The experimentally measured values of the negative Poisson's ratio are in c

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

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

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

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

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

217 In most of the cases, the measured values of the ultrasound-calculated volume achi

218 n-based cohort of American Indian elders had measured values of urine arsenic and cadmium several tim

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

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

221 Pseudoreplication occurs when the number of measured values or data points exceeds the number of gen

222 Our result favours the experimentally measured value over those obtained using the dispersion

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

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

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

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

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

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

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

230 I predictions by the model aligned well with measured values (RMSE 0.57 and nRMSE 10.33%), with a 14.

231 The fact that measured values satisfy lambda 1 has been noted in the c

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

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

234 orders of magnitude closer to experimentally measured values than the compared all-atom and coarse-gr

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

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

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

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

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

240 gy conversion efficiency lower than previous measured values under steady-state conditions.

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

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

243 ce between the ultrasound and the MRI volume measured values was statistically significant.

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

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

246 Measured values were compared with those reported in lit

247 The ultrasound volume measured values were in most of the cases higher than th

248 Measured values were used to derive a predictive equatio

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

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

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

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

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

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

255 imulated grain yields generally matched with measured values (with prediction error ranging from 0 to

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