ライフサイエンスコーパス: MPa

1 f injected vessel files air-seeded below 1.0 MPa, whereas the remainder seeded over a wide range exce

2 ees C under elevated pressures (8.5 and 12.0 MPa) for scCO2-brine, and in limestone and dolomite sand

3 ration at the experimental conditions of 6.0 MPa and 274.2 K for gas hydrate formation.

4 ifferent concentrations was evaluated at 6.0 MPa and 274.2 K.

5 omoter was investigated at 4.5, 5.5, and 6.0 MPa and 274.2 K.

6 2) mol x min(-1) x m(-3) was obtained at 6.0 MPa and 274.2 K.

7 uction times were very low (<3.67 min at 6.0 MPa).

8 d at total pressures in the range of 2.0-8.0 MPa.

9 re, under a small mechanical pressure of 9.0 MPa, and also in ambient.

10 d 12 degrees C for up to 28 days (control--0 MPa) and 42 or 70 days (pressure-treated; 12 and 3.5 deg

11 t the basal part of the plant (0.04 +/- 0.01 MPa), leading to a recovery of conductance (change in pe

12 ally, applied step change in pressure = 0.02 MPa and overall change in volume = 30 pL, respectively)

13 he apical part of the plants; -0.11 +/- 0.02 MPa) and change in percentage loss of conductivity was 0

14 duces the shear stress values to 0.05+/-0.02 MPa.

15 porus) redistributes water from moist (-0.03 MPa) into dry (-9.5 MPa) soil at about 0.3 cm min(-1) in

16 lined most gradually for low (less than 0.08 MPa) pressures and for water inflow and outflow conditio

17 at gamma of 74 mn m(-1) but -2.11 and -2.09 MPa at 45 mn m(-1) This indicates up to about 1 MPa seas

18 nic decrease in PPO activity occurred at 0.1 MPa and pressures higher than 500 MPa.

19 Pd (as suspended Pd/Al2O3 catalyst) and 0.1 MPa H2, pH 3.

20 The mean radius of the AoR, based on a 0.1 MPa pressure change, is around 4.8 km.

21 ort in Shewanella oneidensis at ambient (0.1 MPa) and high (200 MPa) pressure using H/D isotopic cont

22 pared with atmospheric pressure storage (0.1 MPa) at the same temperatures and under refrigeration (4

23 tone and dolomite sands at 23 degrees C (0.1 MPa) for air-brine using a new computer programmed porou

24 with a turnover frequency (0.1 s(-1) at 0.1 MPa, 400 degrees C) an order of magnitude higher than th

25 cosolvent mixtures at T=(298-318)K and p=0.1 MPa.

26 matic excess pressure increase of around 1.1 MPa.

27 ng concentration of 3.6 vol.% approach 119.1 MPa, 5.3 GPa and 2.4 x 10(-4) S m(-1), with increases of

28 epicatechin were similar (35.1 MPa and 22.1 MPa, respectively) and significantly stronger than films

29 ith rutin and epicatechin were similar (35.1 MPa and 22.1 MPa, respectively) and significantly strong

30 With tensile moduli of approximately 9.1 MPa, ultimate tensile strains of approximately 325%, com

31 at 45 mn m(-1) This indicates up to about 1 MPa seasonal variation in 50% loss of hydraulic conducti

32 loss of hydraulic conductivity (-1.7 and -1 MPa for stem and petiole, respectively).

33 Young's modulus was <1 MPa from 5% to 20% strain, before increasing from 20% to

34 sponse to moderate (-0.5 MPa) and severe (-1 MPa) drought stress at the transcriptional, translationa

35 ble upon relaxation of water potential to -1 MPa.

36 reached 48.65 +/- 3.19 MPa and 1.94 +/- 0.10 MPa .

37 d together by the adhesive reach 0.51+/-0.10 MPa, whereas signal-induced depolymerization via quinone

38 200 m and overpressures ( approximately 1-10 MPa) that likely stemmed from conduit blockage.

39 (-1)), and at moderate normal stresses (1-10 MPa), have revealed a complex evolution of the dynamic s

40 material with a Young's modulus of 50 +/- 10 MPa inflated by a turgor pressure estimated to be 1.5 +/

41 ymer materials with stress at break above 10 MPa and melt viscosity lower than 1 Pa.s.

42 ures up to 200 degrees C, pressures above 10 MPa, high salinities, and a pH range from 5-8.

43 h CO2-saturated brine at 50 degrees C and 10 MPa while tomographic images are taken at 15 min interva

44 stone was flooded with brine + scCO(2) at 10 MPa and 60 degrees C parallel to the defect.

45 in, 3 cycles of 1.5 mL water each one) at 10 MPa, a noticeable reduction in extraction time and solve

46 om 10 to <2 MPa) and modulus (from 93 to <10 MPa), increased water vapor permeability (WVP, from 3 to

47 ments (temperature 60 degrees C, pressure 10 MPa).

48 tate were 6% (w/v) of initial substrates, 10 MPa, blend with 30% (w/w) of FHCO and 2h, respectively.

49 latively low strength ([Formula: see text]10 MPa).

50 A large loading of more than 10 MPa can be actuated by a LiFePO4 ||Si full battery with

51 e or nitrogen at elevated pressures up to 10 MPa and temperatures up to 333 K.

52 oid and homogenization pressures (5, 10, 100 MPa).

53 resses in the range of several to almost 100 MPa, largely surpassing those of about 0.3 MPa generated

54 in magma ponding zones, at ~180-200 and ~100 MPa.

55 tic pressure (HP) shock of approximately 100 MPa elicits a RecA-dependent DNA damage (SOS) response i

56 r amount of free fatty acids observed at 100 MPa.

57 ents, where pressures reach the kilobar (100 MPa) range.

58 he oxidative stability of nanoemulsions (100 MPa) and acted synergistically with BHT in increasing th

59 Carotenoid nanoemulsions (100 MPa) were partially (66%) digested and highly bioaccessi

60 sults indicate that, under a pressure of 100 MPa, close to that of the native environment deep under

61 ween 773 K and 923 K and stress range of 100 MPa-300 MPa indicate both a significant improvement of t

62 1000 MPa, and bearable pressure of over 100 MPa.

63 der the sea, where the pressure is up to 100 MPa (1 kbar).

64 h cm(-3), high tensile strength of over 1000 MPa, and bearable pressure of over 100 MPa.

65 om 4 to 12 GPa and hardness from 400 to 1000 MPa.

66 ate compressive strengths up to 1940 +/- 103 MPa were measured at room temperature.

67 d Li attains extremely high strengths of 105 MPa at room temperature and of 35 MPa at 90 degrees C.

68 her than that of UFG-2 steel (sigma y = 1080 MPa and sigma UTS = 1200 MPa), suggesting that the stren

69 tivity at its optimum water potential of -11 MPa.

70 ctor of approximately 360, from 30 kPa to 11 MPa along the first millimeter of the follicle.

71 s of the buckypaper/Parmax composite to 1145 MPa and 150 GPa, respectively, far exceeding those of Pa

72 uptake at water potentials (-41 MPa to -117 MPa) that might occur in putative brines at recurrent sl

73 eel (sigma y = 1080 MPa and sigma UTS = 1200 MPa), suggesting that the strengthening contribution is

74 el had high yield strength (sigma y) of 1260 MPa, and ultimate tensile strength (sigma UTS) of 1400 M

75 s an unexpected increase between 100 and 130 MPa injection pressure.

76 Polygalacturonase was activated at 130 MPa, inactivated reversibly at 330 MPa and activated aga

77 with increasing injection pressure up to 130 MPa, primarily due to the increased small particle aggre

78 proximately 0.6 at 600 degrees C and p = 134 MPa.

79 he microfluidisation pressure from 21 to 138 MPa, resulted in a particle size decrease from 289 to 19

80 ltimate tensile strength (sigma UTS) of 1400 MPa.

81 r seeding pressures ranged from 0.8 +/- 0.15 MPa (mean +/- sd) in the hydric fern Athyrium filix-femi

82 rogels display compressive stresses of 14-15 MPa at 98% compression without fracture or hysteresis up

83 a temperature of 243 K and a pressure of 15 MPa.

84 riaceae, and yeasts/moulds) while at 100/150 MPa, the counts were lower for all the tested temperatur

85 0 and 37 degrees C, under pressure at 25-150 MPa was compared with atmospheric pressure storage (0.1

86 One pass at 150 MPa was the best operating conditions.

87 ean tensile strength ([Formula: see text]150 MPa) and fracture energy ([Formula: see text]350 to 1,24

88 anol, or DMF) or applied pressure (up to 150 MPa) affect the rotational dynamics of encapsulated benz

89 sity reaches saturation at approximately 155 MPa.

90 data over the range of pressure (up to 13.17 MPa), temperature (up to 50 degrees C), and water conten

91 9 GPa, and hardness of approximately 120-170 MPa.

92 stamped with a pressure of approximately 170 MPa in a polycarbonate sample, with a subsequent quantit

93 nisation of the mixture was conducted at 170 MPa for 56 cycles.

94 nd fracture toughness reached 48.65 +/- 3.19 MPa and 1.94 +/- 0.10 MPa .

95 lso oxidized CO at low water potentials (-19 MPa), at temperatures within ranges reported for RSL, an

96 turgor pressure estimated to be 1.5 +/- 0.2 MPa.

97 methods with variations on the order of 1-2 MPa.

98 te (conversion >95% at 100 degrees C and 1.2 MPa for 1.5 h).

99 with young's moduli ranging from 1.8 to 13.2 MPa and extension to failure exceeding 250% over a range

100 increases in collapse from approximately -2 MPa down to -3 MPa, saturating thereafter (to -4 MPa).

101 sured correspond to estimated viscosities >2 MPa s.

102 % to 20%), decreased strength (from 10 to <2 MPa) and modulus (from 93 to <10 MPa), increased water v

103 extensibility (800%), and tensile stress (2 MPa).

104 r temperature and pressure (66 degrees C, 20 MPa) for one week.

105 and KJIc fracture-toughness values above 200 MPa m(1/2); at cryogenic temperatures strength, ductilit

106 lime peel) at ambient pressure, 100 and 200 MPa were used to extract pectin from dried lime peel.

107 remarkable structural changes already at 200 MPa and lost their native functionality.

108 Soymilk was treated at 200 MPa combined with two inlet temperatures (55 or 75 degre

109 a-high pressure homogenisation, UHPH) at 200 MPa did not affect the binding parameters of curcumin to

110 Pasteurisation and UHPH treatments at 200 MPa produced few changes in the volatile composition, re

111 Below 200 MPa and at equivalent depths, the strongly non-ideal beh

112 and fracture toughness values exceeding 200 MPa.m(1/2).

113 and exceptional fracture toughness (KJIc>200 MPa radicalm).

114 neidensis at ambient (0.1 MPa) and high (200 MPa) pressure using H/D isotopic contrast experiments fo

115 must have a modest strength (Earth, </= 200 MPa), but a standard strength profile based on olivine f

116 At pH 8 and pressures higher than 200 MPa, a decrease in total sulfhydryl groups and an increa

117 ibution from 1.9 MPa to 59 MPa and up to 200 MPa, depending on the size of the nanoparticles.

118 e optimal hybrid construct was 3.42 +/- 0.22 MPa.

119 ronger than the novel lightweight steel (227 MPa g(-1) cm(3) ).

120 ncreasing the pressure on the junction to 23 MPa, the photocurrent can be enhanced by a factor of fou

121 The yield strength of 244 MPa and tensile strength of 274 MPa were achieved in the

122 d from a non-focused transducer (1 MHz, 1.25 MPa, PRI 30s) and injection protocols and total amounts

123 investigate the influence of pressure (10-25 MPa) and temperature (20-60 degrees C) in the extraction

124 on yield was obtained at 60 degrees C and 25 MPa, which was 0.47 wt% (run 2).

125 At 25 MPa no microbial inhibition was observed.

126 chanical properties (tensile strength of 250 MPa) are achieved due to the integration of exceptionall

127 %, compressive strengths of approximately 26 MPa, and fracture toughness of as high as approximately

128 300 degrees C with strength in excess of 260 MPa at 250 degrees C.

129 ength of 244 MPa and tensile strength of 274 MPa were achieved in the composite with 0.95 wt.% graphe

130 ure strains up to 90% and KJIc values of 275 MPa m(1/2).

131 ressures, P. profundum grows optimally at 28 MPa and 15 degrees C.

132 ibits a good combination of high modulus (28 MPa), toughness (9300 J m(-3) ), extensibility (800%), a

133 erials reach compressive strengths up to 280 MPa with densities well below 1,000 kg/m(3).

134 0% percent loss of conductance occurring 0.3 MPa earlier than in wild-type plants, and that they also

135 0 MPa, largely surpassing those of about 0.3 MPa generated by contractile muscles.

136 Pulp response of 0.1, 0.2 and 0.3 MPa groups showed only moderate disorganization of the o

137 essure employed is equal or smaller than 0.3 MPa.

138 ) and correspondingly high stress (up to 1.3 MPa) with low density (0.84 g cm(-3)).

139 stem hydraulic conductivity = -1.7 and -1.3 MPa, respectively.

140 erior superior attachment was stiffest (16.3 MPa) and the medial was least stiff (1.4 MPa).

141 rock boundary at 60 degrees C and pCO(2) = 3 MPa using flow-through experiments.

142 ly, the lateral attachment was stiffest (8.3 MPa) and the anterior superior was least stiff (1.4 MPa)

143 nger than films without added phenolics (9.3 MPa).

144 ving optimal conditions of 40 degrees C, 9.3 MPa, and 0.31 molar fraction of CO2 in ethanol.

145 Declines in Kleaf between -2 and -3 MPa were reversible and accompanied by the collapse of t

146 The seasonal Psi varied from 0 to below -3 MPa in both species, with gs and K generally tracking Ps

147 and biaxial tensile strength in excess of 3 MPa, were produced by pulsed current processing.

148 water potentials were more negative than -3 MPa.

149 ollapse from approximately -2 MPa down to -3 MPa, saturating thereafter (to -4 MPa).

150 ract obtained by fractional extraction at 30 MPa and 100 degrees C after the volatile fraction had be

151 t rock cores at effective pressures up to 30 MPa; we then induced a macro-fracture to each sample usi

152 Pressurisation (100-300 MPa) enhanced the hydrolytic efficiency of Protamex, Sav

153 The effect of UHPH at 200 and 300 MPa in combination with different inlet temperatures (Ti

154 ulus and fracture strength of 52 GPa and 300 MPa, respectively.

155 ures (55 or 75 degrees C) and treated at 300 MPa at 80 degrees C inlet temperature.

156 Proteolysis at 300 MPa by Savinase gave rise to lentil hydrolysates (S300)

157 Proteolysis at 300 MPa led to a complete degradation of lentil proteins and

158 UHPH-processing of PC dispersions at 300 MPa was followed by a slight but significant (p=0.05) in

159 K and 923 K and stress range of 100 MPa-300 MPa indicate both a significant improvement of the compo

160 For example, application of 300 MPa and 70 degrees C for 10 min retained 20%, 80% and 65

161 ), an increase in wet modulus from 60 to 300 MPa ( approximately 500% increase) is observed after pho

162 e from 219 K to 473 K and pressure up to 300 MPa.

163 2 degrees C in soymilk treated by UHPH (300 MPa and 75 degrees C of inlet temperature) were studied

164 0% of DCC was increased from 69.63 to 125.31 MPa.

165 trasound (551.5 kHz focused transducer, 0.33 MPa average peak rarefaction pressure) in the presence o

166 ed at 130 MPa, inactivated reversibly at 330 MPa and activated again at 530 MPa.

167 ously reported strengths being less than 340 MPa at 1500 degrees C or above.

168 ths of 105 MPa at room temperature and of 35 MPa at 90 degrees C.

169 eated raw almond milk (AMr) with UHPH at 350 MPa and 85 degrees C (AMuhph), known able to inactivate

170 s a mechanical tensile strength of up to 350 MPa, nearly three times of that of a film with randomly

171 ery low contact stresses (between 1.1 and 38 MPa).

172 6.3 MPa) and the medial was least stiff (1.4 MPa).

173 d the anterior superior was least stiff (1.4 MPa).

174 perature with a recovered tensile strength 4 MPa, which is 30% of its original value, yet comparable

175 down to -3 MPa, saturating thereafter (to -4 MPa).

176 ressure-mild temperature conditions (0.1-400 MPa, 60 degrees C) also caused up to 3 fold PPO activity

177 and mild pressure-high temperature (0.1-400 MPa, 70-80 degrees C) combinations.

178 at combinations of lower pressures (200-400 MPa) and high temperatures (60-80 degrees C), there was

179 , application of moderate pressures (200-400 MPa) can potentially be used to retain myrosinase activi

180 Hc when increasing pressure from 200 and 400 MPa to 600 MPa.

181 but fully preserved after HPP at 200 and 400 MPa.

182 This phase forms at approximately 400 MPa and 280 K with the nominal composition (H2O)2H2 and

183 (min) for Igs ranged from 4941 to 452 at 400 MPa and from 235 to 40 at 600 MPa.

184 Pressure at 400 MPa was found to be the threshold for loss of solubility

185 effect of high pressure (HP) treatment (400 MPa, 10 min) of porcine longissimus dorsi was investigat

186 gnificantly increased by annealing under 400 MPa/60 degrees C pressure for 15 min followed by resting

187 of active CO uptake at water potentials (-41 MPa to -117 MPa) that might occur in putative brines at

188 at this energy level, and peak pressure (41 MPa) and maximum cavitation activity were both realigned

189 he wines were pressurised at 500 MPa and 425 MPa for 5 min.

190 tical resolved shear stress (CRSS) is ~33-43 MPa, ~10 times higher than that of pure nickel.

191 ites by ~75% (5.60 MPa.m(1/2)) and ~25% (430 MPa), respectively, compared with those of pure Al2O3.

192 tlp was widely prevalent but moderate (-0.44 MPa), accounting for 16% of post-drought pitlp.

193 he same ultrasound parameters (1 MHz at 0.45 MPa and 10 Hz with 10% duty cycle), PUT with 4 mJ/cm(2)

194 echanical properties (tensile stress of 1.45 MPa, tensile strain of approximately 600%, and fracture

195 -pressure processing (HPP) (150, 300 and 450 MPa for 0, 2.5 and 5 min) on total sodium dodecyl sulpha

196 Structural changes by HHP (450 MPa for 3 and 5 min) improve thermal stability of wine p

197 us, application of the highest pressure (450 MPa) provoked a significant degradation of phosphoglycer

198 creased their intensity after applying a 450-MPa processing.

199 A treatment of 453 MPa for 5 min with a 2.5% (w/v) of Stevia succeeded in i

200 The Young's modulus (1.47 MPa) and hydrophobicity (with a sessile drop contact ang

201 Results differ by less than 0.5 MPa on average, in contrast to comparison between conven

202 cv. RB867515), in response to moderate (-0.5 MPa) and severe (-1 MPa) drought stress at the transcrip

203 supercritical CO(2) at 51 degrees C and 19.5 MPa to access the reactivity of these formations at stor

204 rties, such as higher tensile strength (27.5 MPa) and elongation at break (17.9%), than those composi

205 ane hydrates grow under mild conditions (3.5 MPa and 2 degrees C), with faster kinetics (within minut

206 and then in older, coarse roots (P50 = -3.5 MPa).

207 show a large range in P50 from -0.5 to -7.5 MPa, which overlaps with 94% of the woody angiosperm spe

208 water from moist (-0.03 MPa) into dry (-9.5 MPa) soil at about 0.3 cm min(-1) in single hyphae, resu

209 mainder seeded over a wide range exceeding 5 MPa.

210 respectively, and an operating pressure of 5 MPa (50 bar).

211 h intra-annual fluctuations reaching up to 5 MPa.

212 ime with the critical point at ~207 K and 50 MPa.

213 Under the same operative conditions (50 MPa, 86 degrees C, 4 mL min(-1) SC-CO2 flow) extraction

214 high pressure processing treatment (300-500 MPa, 5-15 min) combined with Stevia rebaudiana (Stevia)

215 Samples were pressure-treated at 300 and 500 MPa and stored at 3.5 and 12 degrees C for up to 70 days

216 Samples were pressure-treated at 300 and 500 MPa and were stored at 3.5 and 12 degrees C for up to 28

217 dispersions and mixtures were treated at 500 MPa (pH 7.0 and 5.8) at room temperature, -15 degrees C

218 e with a maximum of 6.1 fold increase at 500 MPa and 30 degrees C.

219 mentation, the wines were pressurised at 500 MPa and 425 MPa for 5 min.

220 indicate that exposure to helium gas at 500 MPa leads to a stoichiometry close to (He1 square1)(CaZr

221 red at 0.1 MPa and pressures higher than 500 MPa.

222 Purees were subjected to HPP (130-530 MPa) under quasi-isobaric non-isothermal conditions (15

223 rsibly at 330 MPa and activated again at 530 MPa.

224 nly 4 kg (9 lbs) and could generate up to 55 MPa (8000 psi) pressure.

225 Cell stiffness was 0.56 MPa, consistent with cells possessing a cell wall.

226 lows a broad distribution from 1.9 MPa to 59 MPa and up to 200 MPa, depending on the size of the nano

227 strength of the macrofiber is as high as 598 MPa g(-1) cm(3) , which is even substantially stronger t

228 rted forming under mild drought stress (-0.6 MPa Psistem), coincided with a dramatic reduction in Lpr

229 he combination of small diameter MBs and 0.6 MPa US also resulted in significantly greater gene expre

230 a-CD) powder on CO2 encapsulation at 0.4-1.6 MPa pressure for 1-72 h through the addition of water (t

231 D) powders, under various pressures (0.4-1.6 MPa) and time periods (4-96 h).

232 ose composites containing only AMO-LDH (25.6 MPa and 7.5%, respectively).

233 h yield strength and elongation of 276 +/- 6 MPa and 34.3 +/- 3.4% respectively.

234 a good fracture toughness (K1C) of 23.5-29.6 MPa m(1/2) were obtained in high-carbon martensitic stee

235 rated medium with a water potential of -39.6 MPa; activity was reduced by only 28% relative to activi

236 ea resistance was variable but averaged 54.6 MPa s m(-1) across all surveyed pteridophytes.

237 0 degrees C were pressed into flakes under 6 MPa and sintered at 1400 degrees C, the resulting flakes

238 gth (sigmaf) of the composites by ~75% (5.60 MPa.m(1/2)) and ~25% (430 MPa), respectively, compared w

239 an average ultimate tensile strength of 6.60 MPa and an average failure strain of 4.18%.

240 ogy analysis indicated that HHP at 40 and 60 MPa promoted embryo competence through down-regulation o

241 vely high pressure-mild temperature (400-600 MPa, 60 degrees C) and mild pressure-high temperature (0

242 The treatments at 400 and 600 MPa for 3 min maintained the volatile compounds at simil

243 high-pressure processing--HPP--(450 and 600 MPa/3 min/20 degrees C) on the colour, carotenoids, asco

244 The pressure treatments at 600 MPa for 15 and 30 min led to similar or higher losses th

245 HPP at 600 MPa for 2.5 min resulted in the maintenance of IgA and l

246 to 452 at 400 MPa and from 235 to 40 at 600 MPa.

247 ty were obtained when HPP was applied at 600 MPa.

248 However, the application of 600 MPa for 6 min changed the original volatile compounds of

249 Since, HPP at 400 or 600 MPa for 3 min preserved the original volatile compounds

250 min) or high-pressure treatments (400 or 600 MPa for 3 or 6 min) on the volatile compound profile of

251 ha-helix and random coil contents of the 600 MPa treated samples were 23.67% and 37.54%, respectively

252 reasing pressure from 200 and 400 MPa to 600 MPa.

253 tly influenced by HP or HPHT treatments (625 MPa; 5 min; 20, 70 and 117 degrees C).

254 apparatus at 40 degrees C and 1400 psi (9.65 MPa).

255 the pressure was increased from 13.8 to 20.7 MPa.

256 ure, and pressing duration were 5% d.b., 9.7 MPa and 4 min, respectively, with a defatting ratio of 7

257 grees C combined with 0.1 to 700 MPa and 700 MPa combined with 85-115 degrees C) on beta-carotene iso

258 became almost temperature insensitive at 700 MPa.

259 sing (100 degrees C combined with 0.1 to 700 MPa and 700 MPa combined with 85-115 degrees C) on beta-

260 to 80 degrees C and pressure from 0.1 to 700 MPa.

261 trength of the resultant fibers reaches ~729 MPa after a super high temperature thermal annealing tre

262 rated condition, hyperbaric storage at 50/75 MPa resulted in similar or lower microbial counts (total

263 migration under confinement in a stiff (1.77 MPa) environment, we use soft lithography to fabricate p

264 a-CD at low pressure and short time (0.4-0.8 MPa and 4-24 h), but was markedly enhanced with an incre

265 ydraulic conductance [kleaf] at -0.2 to -0.8 MPa).

266 hydraulic conductivity [P50] reached at -1.8 MPa) and then in older, coarse roots (P50 = -3.5 MPa).

267 oss the Callitris clade (P50 : -3.8 to -18.8 MPa), and was significantly related to water scarcity, a

268 with a tensile modulus of approximately 4-8 MPa.

269 for one to six months at 65 degrees C and 8 MPa Ptotal.

270 nate at high salinity and at a pressure of 8 MPa, with results comparable to those observed when grow

271 ysts with three different HHP (40, 60 and 80 MPa) in combination with three recovery periods (0, 1 h,

272 ficantly higher at 40 and 60 but lower at 80 MPa after vitrification-warming in the treated groups th

273 In contrast, 80 MPa up-regulated genes in apoptosis, and down-regulated

274 s observed with increasing pressure (400-800 MPa), temperature (5-40 degrees C) and time (0-60 min).

275 J mol(-1) within the pressure range (500-800 MPa) indicating high independence on the temperature at

276 nactivation increased with pressure (600-800 MPa) and temperature (30-70 degrees C) for all the musta

277 rk meat pressurised at 200, 400, 600, or 800 MPa (10 min, 5 or 20 degrees C).

278 gums and those treated at high pressure (800 MPa) both at their "natural" pH (4.49 and 4.58, respecti

279 rms and after exposure to high pressure (800 MPa).

280 2 ceramics can be increased to more than 800 MPa at temperatures in the range of 1500-2100 degrees C.

281 bers yield record high tensile strength (826 MPa) and Young's modulus (65.7 GPa) owing to the large l

282 antile, 50% of K was lost at -2.58 and -3.84 MPa in P. munitum and D. arguta, respectively.

283 human bone) and high ultimate strength (853 MPa) was fabricated.

284 in P. abies and P. mugo was -3.35 and -3.86 MPa at gamma of 74 mn m(-1) but -2.11 and -2.09 MPa at 4

285 odulus follows a broad distribution from 1.9 MPa to 59 MPa and up to 200 MPa, depending on the size o

286 g from 20% to 50% strain to a maximum of 2.9 MPa.

287 a mechanical shear strength higher than 8.9 MPa.

288 of 50 degrees C and two pressures: 4.2 and 9 MPa.

289 observed with extracts obtained by SFE at 9 MPa.

290 ssive flow strengths ranging from 500 to 900 MPa have been obtained.

291 c fern Athyrium filix-femina to 4.9 +/- 0.94 MPa in Psilotum nudum, an epiphytic species.

292 ile strength of the film from 70.02 to 97.97 MPa.

293 genated amorphous silicon can be produced at MPa pressures from silane without the use of plasma at t

294 membrane flux ranged between 80 and 276 LMH/MPa, roughly 4-10 times higher than that of most commerc

295 and tooth pressures (718-2,974 megapascals [MPa]) promoting crack propagation in bones, (2) tooth fo

296 filament compliance (Cf) of 13.1 +/- 1.2 nm MPa(-1), close to recent estimates from single fibre mec

297 from single fibre mechanics (12.8 +/- 0.5 nm MPa(-1)).

298 vol% that exhibit strengths of the order of MPa (three orders of magnitude higher than the interfaci

299 onfinement, which was found to reach tens of MPa inside submicron bubbles.

300 Early PCR diagnostic tests focused on the MPa adhesion gene and the 16S ribosomal RNA gene.