ライフサイエンスコーパス: MPa

1 hat applied pressures of much greater than 0 MPa were required to induce water release from the xylem

2 gged and stem water potential was close to 0 MPa, and in leafless saplings over the winter period.

3 gth was controlled, ranging from 0.14+/-0.01 MPa to 20.17+/-2.18 MPa, and strain was varied from 11.8

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

5 or CA/Gel/Beri nanofibers were 2.69 +/- 0.05 MPa, 56.93 +/- 1 degrees , 76.17 +/- 0.76%, 10.17 +/- 0.

6 to VF (82 +/- 19 MPa) and PFD (1.6 +/- 0.06 MPa).

7 g in-plane (~7 MPa) and out-of-plane (<=0.08 MPa) directions.

8 CA/Gel nanofibers were around 2.83 +/- 0.08 MPa, 58.07 +/- 2.35 degrees , 78.17 +/- 1.04%, 11.23 +/-

9 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

10 K(Ic) is determined to be ~0.1 MPa m(0.5), which is even lower than that of brittle oxi

11 as carried out in a fixed bed reactor at 0.1 MPa over a temperature range of 275-375 degrees C.

12 id-bearing MBs with pulsed low-pressure (0.1 MPa) 1.1-MHz FUS facilitates sonoselective gene delivery

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

14 avior with a Young's modulus of 0.33 +/- 0.1 MPa, very similar to that of native peripheral nerve.

15 of methane and propane at pressures near 0.1 MPa.

16 tress reduction of 50% (values of 1.2 to 1.1 MPa).

17 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

18 arcy, mD) immediately after fracture (at 2.1 MPa confining pressure).

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

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

21 low values typical of linear polymer CANs (1 MPa).

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

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

24 (U ~ 1.4 MJ.m(-3)), and strengths (sigma ~ 1 MPa).

25 resistance (1,000 J/m(2)), high strength (1 MPa), low Young's modulus (100 kPa), and high water cont

26 tances up to 0.5 m, and stress-drops up to 1 MPa, which are comparable to observed values of moderate

27 r 10 MPa, 70 degrees C, then ethanol 48%, 10 MPa, 70 degrees C), varied between 5 and 15 g/kg dry wei

28 as the shear modulus varies between 1 and 10 MPa and the stress relaxation by 2 orders of magnitude.

29 es (200, 350 and 500 MPa of HHP; 4, 7 and 10 MPa of HPCD) were compared by evaluating the texture, co

30 the corresponding dry adsorbed amount at 10 MPa.

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

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

33 hemispheres (modulus ranging from 0.7 to 10 MPa) on 4 different polycrystalline diamond substrates w

34 phenylalanine) in the driest treatment (-10 MPa) were similar in both soils regardless of amendment

35 orage on the dry Cr-soc-MOF-1 (<=3 MPa vs 10 MPa).

36 tial pressurized liquid extraction (water 10 MPa, 70 degrees C, then ethanol 48%, 10 MPa, 70 degrees

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

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

39 s much higher than that induced by HP at 100 MPa (HP100, 12 mum), followed by an endoprotease with hi

40 ve high-resolution two-photon imaging at 100 MPa of living microbes from all three kingdoms of life.

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

42 fting the onset of protein unfolding by ~100 MPa.

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

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

45 1000 MPa, and bearable pressure of over 100 MPa.

46 ation-tolerant (DT) plants can dry past -100 MPa and subsequently recover function upon rehydration.

47 h of the scaffold decreasing from 180 to 100 MPa in 6 weeks, which is still sufficient for load-beari

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

49 site delivers a yield strength of up to 1000 MPa, plasticity over 10%, and Young's modulus of approxi

50 a unique combination of high strength (1010 MPa), high toughness (62 MJ m(-3) ) and high stiffness (

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

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

53 re exhibits a tensile yield strength of 1074 MPa with a reasonable ductility of 8%.

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

55 Improved tensile strength (73 +/- 11 MPa) in machine produced structures is due to alignment

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

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

58 The ultimate tensile strength was 1165 MPa with ductility of ~18% and ultimate compressive stre

59 s experienced differential stresses of ~3-12 MPa, consistent with their storage in mush piles with th

60 papers stayed constant at ~ 14 GPa and ~ 120 MPa, respectively.

61 )pyridine] at applied pressures of up to 120 MPa (1200 bar).

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

63 sed 1, 2 and 3 times through 75, 100 and 125 MPa pressures.

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

65 pe tip, generating a growth stress up to 130 MPa; this value is substantially higher than the stresse

66 hardness (32.4 GPa), dynamic strength (1323 MPa), strain and toughness were determined for the sampl

67 n at a reservoir pressure threshold of 12-14 MPa regardless of assumed model rheology, lending suppor

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

69 oy show relatively high flow-stresses, ~1400 MPa under quasi-static loading and in excess of 1800 MPa

70 There was studied the influence of HPH (150 MPa) and pasteurization (92 degrees C for 30 s and 85 de

71 The highest strength of ~150 MPa (which is 95.2% higher than that of the flat YSZ/Ti6

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

73 films display high tensile strength (134-158 MPa), stretchability (~ 26% elongation), and high toughn

74 nificant increase of yield strength from 159 MPa (T4) to 270 MPa (T6).

75 h enhanced shear adhesive strengths up to 16 MPa, while alloying with commercial core-shell particle-

76 9 GPa, and hardness of approximately 120-170 MPa.

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

78 ranging from 0.14+/-0.01 MPa to 20.17+/-2.18 MPa, and strain was varied from 11.85+/-0.88 % to 51.20+

79 r quasi-static loading and in excess of 1800 MPa under dynamic loading.

80 % and ultimate compressive strength was 1863 MPa with a total compressive fracture strain of ~34%.

81 network formation compared to VF (82 +/- 19 MPa) and PFD (1.6 +/- 0.06 MPa).

82 asing to 0.25 x 10(-15) m(2) (0.25 mD) at 19 MPa confining pressure (approximately 800 m depth), and

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

84 otosynthesis in trees continues down to -1.2 MPa or lower, depending on species and measurement metho

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

86 y reduced the polymerization stress from 2.2 MPa to 1.7 to 1.4 MPa, resulting in 20% stress reduction

87 d and xylem water potential declined to -3.2 MPa on average, causing a 46% loss of stem hydraulic con

88 to 33 GPa) and fracture toughness (up to 5.2 MPa.m(1/2)), significantly surpassing expected values fr

89 lity (> 35% strain), low Young's modulus (~2 MPa), superior mechanical, electrical and electrochemica

90 n appreciable compressive strength beyond 20 MPa, which was ~2-fold higher than that of pure CSi scaf

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

92 (7.8 GPa) than pure polymer electrolytes (20 MPa).

93 y resins led to shear strengths exceeding 20 MPa.

94 rocks, at normal effective stresses up to 20 MPa, with a slip-rate ranging between 10 mum/s and 1 m/s

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

96 ge especially for the samples treated at 200 MPa after 2 months, comparable to the thermal treated on

97 med that "Laba" garlic treated by HHP at 200 MPa was most acceptable to consumers.

98 results indicated that HHP treatment at 200 MPa was optimal for retaining the textural quality of "L

99 and extraordinary mechanical strength (>200 MPa) and a low apparent particle expansion of ~40% upon

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

101 Highest tensile strength (87 +/- 21 MPa) was recorded for CS structures, indicating a more h

102 cantly enhances tensile strength to over 210 MPa while maintaining elasticity.

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

104 trongest (S(f) = 21 mN/tex, or sigma(f) ~ 22 MPa) and stiffest (J = 300 mN/tex, or E ~ 320 MPa) self-

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

106 High pressures (120 and 240 MPa) and added ethanol resulted in change in casein hydr

107 re mechanical loading reaches as high as 244 MPa.

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

109 e, under a constant confining pressure of 25 MPa, are used to elucidate the initiation, growth, and c

110 The best defined extraction condition was 25 MPa, 433.15 K, and 20% H(2)O, with 30.69% of the total y

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

112 %, compressive strengths of approximately 26 MPa, and fracture toughness of as high as approximately

113 300 degrees C with strength in excess of 260 MPa at 250 degrees C.

114 mability (7.8 mm) and T6 yield strength (270 MPa) in this new magnesium alloy is comparable to that o

115 e of yield strength from 159 MPa (T4) to 270 MPa (T6).

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

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

118 itude higher than pristine MXene films of 29 MPa) while still maintaining a high capacitance of 298 F

119 itions ([W] 12.2 +/- 0.6%d.b., [P] 6 +/- 0.3 MPa and time [t] 18.2 +/- 0.6 min).

120 essure employed is equal or smaller than 0.3 MPa.

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

122 The high Young's modulus, 20.3 MPa, and excellent photothermal performance render repea

123 reafter decreases abruptly by 1,200 psi (8.3 MPa) over 370 ft (113 m) as the main sandstone reservoir

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

125 d phase storage on the dry Cr-soc-MOF-1 (<=3 MPa vs 10 MPa).

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

127 urements under the activity test pressure (3 MPa) reveal that the CO(2) hydrogenation to methanol on

128 S pressure, with higher pressures (i.e., 0.3-MPa and 0.4-MPa FUS) consistently inducing BBB opening a

129 or a pressure change of only 0-300 bar (0-30 MPa), an adiabatic temperature change of 3 K is observed

130 e, and SFE was carried out for 210 min at 30 MPa, 55 degrees C and 15% ethanol-water as cosolvent.

131 At high confining pressures (30 MPa), permeability changes were more sensitive to the me

132 llite (IMt-2)-using CO(2) and CH(4) up to 30 MPa at 25-115 degrees C.

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

134 talline discs at 200 degrees C and about 300 MPa of uniaxial pressure.

135 PPO (57%) was achieved with 600 MPa and 300 MPa applied in three cycles, respectively what indicates

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

137 ty was continuously processed by UHPH at 300 MPa (inlet temperature: 23-25 degrees C).

138 in following high pressure processing at 300 MPa for 15 min at 10 and 80 degrees C.

139 HPP at 300 MPa in three cycles caused the highest carotenoids degra

140 dase (PPO) enzymes (57%) was obtained at 300 MPa x 3 pulses, and peroxidase (POD) enzymes (31%) at 60

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

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

143 HP treatment back and forth up to ~300 MPa causes irreversible covalent oligomerization of BLG.

144 observed in situ under pressures up to ~300 MPa: either a complete protein unfolding, from native di

145 hem to yield at 130 +/- 45 MPa and 96 +/- 31 MPa respectively, with significant strain hardening.

146 Pa) and stiffest (J = 300 mN/tex, or E ~ 320 MPa) self-healing polymers able to repair under typical

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

148 a remarkably high mechanical strength of 341 MPa (an order of magnitude higher than pristine MXene fi

149 operties with a high tensile strength of 342 MPa and a Young's modulus of 43.6 GPa, respectively.

150 z; five cycles; peak negative pressure, 0.35 MPa) of ultrasound emitted at a rapid rate (1.25 kHz) in

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

152 rticles operated at a maximum pressure of 35 MPa.

153 yet their strength is roughly less than 350 MPa.

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

155 e day, with Suc contributing ~50% of the 0.4 MPa diurnal osmotic adjustment.

156 +/- 0.5 MPa) compared to CENP-A (6.2 +/- 0.4 MPa) and H3 (9.8 +/- 0.7 MPa) and that the dynamics of b

157 loss of conductivity at lower tension (~0.4 MPa) in grapevine.

158 merization stress from 2.2 MPa to 1.7 to 1.4 MPa, resulting in 20% stress reduction.

159 Active films had higher TS (13.4 MPa) and lower WS (62.8%).

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

161 with higher pressures (i.e., 0.3-MPa and 0.4-MPa FUS) consistently inducing BBB opening and extravasc

162 ercritical CO(2) (SC-CO(2)) pressures (10-40 MPa) on phenolic compounds extraction in oils obtained f

163 droxymatairesinol, particularly at 30 and 40 MPa, while 3-vinylphenol was the predominant compound in

164 a fruit as affected by HHP treatment (50-400 MPa for 3-60 min) and during subsequent storage at 4 deg

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

166 t 500 and 600 MPa at 20 degrees C and at 400 MPa at 50 degrees C.

167 ed that high hydrostatic pressure (HHP) (400 MPa for 5 min) induced the transfer of folic acid and ph

168 For both species, 400 MPa and thermal treatment were the most effective in the

169 Among the tested treatments, 400 MPa may be considered as the best option for the quality

170 y outcome at the lowest pressure level, 0.43 MPa, was on average 1.8-fold and 3.7-fold higher than th

171 me was employed (220 kHz frequency, and 0.44 MPa peak-to-peak pressures) for 30 min.

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

173 in xylem resistance to embolism, with a 1.45 MPa variation in the water potential at which 50% of the

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

175 h nanoboxes show them to yield at 130 +/- 45 MPa and 96 +/- 31 MPa respectively, with significant str

176 uding resistant starch (RS), whereas 150-450 MPa significantly increased RS, without modifying IDF/SD

177 Extraction at 450 MPa and 60% hexane concentration in the solvent mixture

178 protein-cell wall fiber formed at HHP <= 450 MPa.

179 emonstrate that hydrostatic pressures of 450 MPa are sufficient to completely dissociate the Bfr 24-m

180 Pressurization (450 MPa/5 min) significantly enhanced the anti-ACE (14.09 mg

181 compared to ultra-fine grain structure (~450 MPa) concurrent with high uniform tensile ductility (~35

182 ned in one of the conditions is close to 450 MPa m(3)/mg, which is about 22% to 85% greater than any

183 HHP-treated 'Weiki' (450 MPa/5 min and 650 MPa/5 min) was the most potent inhibit

184 61.97-14.48 mg/mL), HHP-treated 'Weiki' (450 MPa/5 min) showed the highest anti-AGE activity (12.37 m

185 h stops at soil moisture potentials of -0.47 MPa for larch and -0.66 MPa for spruce, whereas photosyn

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

187 esses during pushoff increased from 41 to 48 MPa as walking speed was increased, and were comparable

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

189 has an intermediate elasticity (8.5 +/- 0.5 MPa) compared to CENP-A (6.2 +/- 0.4 MPa) and H3 (9.8 +/

190 , as the pressure increased from 0.02 to 0.5 MPa.

191 Sample pressures ranged from 0.02 to 0.5 MPa.

192 High-pressure (1.1-15.5 MPa) column and batch experiments were conducted at a ra

193 icular cartilage explants were loaded to 2.5 MPa (physiological) or 7 MPa (non-physiological) (1 Hz,

194 loss of K(shoot) occurring at -1.7 and -2.5 MPa in S. haematodes and S. pulcherrima, respectively.

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

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

197 rs of magnitude at low confining pressure (5 MPa).

198 film roughness at pressures between 1 and 50 MPa.

199 ions of silicon at extreme pressures of ~ 50 MPa (~ 500 atm) have been observed to generate remarkabl

200 ferent treatment pressures (200, 350 and 500 MPa of HHP; 4, 7 and 10 MPa of HPCD) were compared by ev

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

202 a oneidensis bacteria at pressures up to 500 MPa using quasi-elastic neutron scattering (QENS).

203 ccepted by the crystal pressure value of 550 MPa is reported.

204 -fold and 3.7-fold higher than those at 0.56 MPa and 0.70 MPa, respectively.

205 jury occurred at pressures from 0.39 to 0.56 MPa.

206 monstrate record tensile strength up to ~570 MPa for a 940 nm thick film and electrical conductivity

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

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

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

210 2 degrees C and soil water potential > -0.6 MPa).

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

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

213 ry scores were reached at low pressures (4-6 MPa).

214 olized xylem area occurring at -3.0 and -4.6 MPa in S. haematodes and S. pulcherrima, respectively.

215 0 degrees C were pressed into flakes under 6 MPa and sintered at 1400 degrees C, the resulting flakes

216 70-75%) and low bulk strength (10(-4)-10(-6) MPa); however, the nature and physical properties of the

217 003 (control), -0.15, -0.30, -0.45 and -0.60 MPa.

218 600 MPa-treatment induced the maximum BS-binding ability and

219 s of high pressure treatments (200, 400, 600 MPa for 5 min) and a thermal treatment (85 degrees C for

220 when the protein was treated at 500 and 600 MPa at 20 degrees C and at 400 MPa at 50 degrees C.

221 fugation was pressure-treated at 400 and 600 MPa for 5 and 10 min, and centrifuged to generate granul

222 gh hydrostatic pressure (0, 200, 400 and 600 MPa) was examined.

223 decreased in samples exposed to 400 and 600 MPa.

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

225 h specificity (Tail21, 8 mum), and HP at 600 MPa (HP600, 5 mum).

226 The flash HPT treatment applied at 600 MPa and at 0 degrees C could be the best choice to prese

227 overy in P(P) fractions, specifically at 600 MPa for 10 min, which had the highest value of phosvitin

228 The exposure at 600 MPa led to washed muscle oxidation even in the absence o

229 s, and peroxidase (POD) enzymes (31%) at 600 MPa working in static mode.

230 tarch of OS was partially gelatinized at 600 MPa.

231 lowest degradation (26%) was achieved at 600 MPa.

232 HT and HHP-600 MPa led to significant IDF reduction, including resistan

233 The pressure of 600 MPa caused significant decreases in peak viscosity, brea

234 CN (from 0 to 5 mg/mL) were pressurized (600 MPa-5 min).

235 x and starch granules more severely than 600 MPa; however, tightly-packed complexes of globular starc

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

237 tion occurred in PD and Red subjected to 600 MPa.

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

239 OD (31%) and PPO (57%) was achieved with 600 MPa and 300 MPa applied in three cycles, respectively wh

240 ure demonstrated higher yield strength (~620 MPa) compared to ultra-fine grain structure (~450 MPa) c

241 ng the pit was 0.894 MPa for stems and 0.644 MPa for roots, although considerable variation was appar

242 robust ultrahigh-pressure operation up to 65 MPa.

243 HHP-treated 'Weiki' (450 MPa/5 min and 650 MPa/5 min) was the most potent inhibitor of AGEs in the

244 potentials of -0.47 MPa for larch and -0.66 MPa for spruce, whereas photosynthesis in trees continue

245 tance (100 washing cycles), and strength (68 MPa), these fibers have an energy density of 306 muWh cm

246 CENP-A (6.2 +/- 0.4 MPa) and H3 (9.8 +/- 0.7 MPa) and that the dynamics of both canonical and CENP-A

247 estimates of midday turgor were always >0.7 MPa.

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

249 ~40%, for applied pressures between 0 and ~7 MPa.

250 decrease with increasing pressure beyond ~7 MPa.

251 0%), elasticity, and low Young's modulus (<7 MPa).

252 were loaded to 2.5 MPa (physiological) or 7 MPa (non-physiological) (1 Hz, 15 min) and mechanically-

253 dhesive strength when comparing in-plane (~7 MPa) and out-of-plane (<=0.08 MPa) directions.

254 o detected Achilles tendon loading of 4 to 7 MPa in late swing.

255 -fold higher than those at 0.56 MPa and 0.70 MPa, respectively.

256 5 mum particle-packed columns operated at 70 MPa were compared to conventional ion-chromatography tec

257 lined stainless steel columns operated at 70 MPa, and effects of thermal gradients on separation effi

258 (up to 150 degrees C) and high pressure (70 MPa).

259 ent viscosity (AV) at 150 degrees C under 70 MPa pressure, as compared to drilling fluids that were f

260 iable combinations of pressure (up to 82.727 MPa) and temperature (up to 121.1 degrees C).

261 ia uniaxial tensile elongation analysis (~75 MPa).

262 d bamboo leads to a specific strength of 777 MPa cm(3) g(-1) , which is significantly greater than ot

263 e ultimate tensile strength 646.69 +/- 12.79 MPa and Zn-0.8Li-0.8Mn alloy with elongation 103.27 +/-

264 espite a decrease in water potential to -1.8 MPa at midday.

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

266 a continuously increased strength up to 13.8 MPa, surpassing the original strength of all other count

267 a tensile strength and toughness up to 14.8 MPa and 87.0 MJ m(-3) , respectively.

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

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

270 the optimal parameters (40.2 degrees C, 43.8 MPa and time 30 min), the oil yield was 14.5 g.100 g(-1)

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

272 of different treatments between 200, and 800 MPa at low initial temperatures (between -15, and 50 deg

273 s did not induce changes in Igs while at 800 MPa, all combinations reduced the control levels.

274 2 ceramics can be increased to more than 800 MPa at temperatures in the range of 1500-2100 degrees C.

275 en flexural strength (varying from 89 to 800 MPa) and fracture toughness (varying from 4 to more than

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

277 n instant recovered tensile strength of 1.84 MPa and a continuously increased strength up to 13.8 MPa

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

279 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

280 31.3 MHz and a peak-to-peak pressure of 1.87 MPa, as measured at 1.5 mm from the probe.

281 with strength varying over the range 90-880 MPa, modulus varying over the range 14-116 GPa, and dens

282 ssure required for sealing the pit was 0.894 MPa for stems and 0.644 MPa for roots, although consider

283 The fibre exhibits a tensile strength of 895 MPa and a stretchability of 44.3%, achieving mechanical

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

285 ansplantation in C57/B6 mice, pFUS (PNP: 2.9 MPa, I(sptp): 895 W/cm(2)) improved the function of tran

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

287 tion compared to cross directional (43 +/- 9 MPa) fractured structures as shown in our Scanning Elect

288 ure toughness (varying from 4 to more than 9 MPa.m(1/2)).

289 e, retaining high tensile yield stress (~900 MPa) with appreciable tensile ductility (>20%), via anne

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

291 high longitudinal tensile strength of 91.95 MPa and toughness of 2.73 MJ m(-3)) of the aesthetic woo

292 creased tensile strength (from 22.71 to 3.97 MPa), increased water vapor permeability (from 3.62 to 4

293 The tensile strength and Young's modulus at MPa levels are comparable or even higher than chemically

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

295 Pa, orders-of-magnitude less than those (few MPa) obtained by tensile/inflation testing.

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

297 which results in high sensitivity (~5.59 mV MPa(-1) ), giant switching (>10(5) ), and fast response

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

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

300 ntifouling properties were also tested under MPa compression pressures by direct force measurements u