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1 a higher density in the capsid with a higher internal pressure.
2 he capsid with DNA and encounters increasing internal pressure.
3 nsequently, its absence results in increased internal pressure.
4 y to tune their contractility in response to internal pressure.
5 gether enable the polymer chips to withstand internal pressures above 20 MPa (approximately 2900 psi)
6                We investigate the effects of internal pressure and actuator temperature as control in
7       This condensation modulates the virion internal pressure and DNA release from disrupted particl
8  constrained expansion, increasing notochord internal pressure and driving its elongation and stiffen
9 ontrols the bonding strength by changing its internal pressure and exploiting the mechanics of interf
10 ors, allowing for the acquisition of data on internal pressure and more sophisticated pyrolysis analy
11 astic modulus and failure mode dependence on internal pressure and on wall integrity are borne out by
12                        Their size, shape and internal pressure are determined by the competition betw
13 cuffs' outer diameter, length, material, and internal pressure are the main determinants of sealing e
14              These capsids can stand with an internal pressure as high as approximately 50 atmosphere
15 ed by local zeta potential control induce an internal pressure at the microchannel intersection, resu
16 ing, flattening of the vesicle increases the internal pressure beyond the bursting point.
17  Language processing is hastened not only by internal pressures but also externally by turn-taking in
18          The walls are rigid to resist large internal pressures, but remarkably plastic to adapt to a
19        We show that these shells can relieve internal pressure by bursting intermittently, shrinking
20 r beneath the volcano's summit, reducing its internal pressure by ~17 megapascals.
21 ith periodic holes by incorporating a single internal pressure cavity.
22 n upon swelling generates tensile stress and internal pressure, contributing to volume changes in bio
23 nditions may have resulted in a large enough internal pressure decrease to promote the metastable cry
24 nitor genome loss upon heating, we find that internal pressure destabilizes the virion, resulting in
25 yzer cell with a strong metal structure, for internal pressure difference of up to 100 bar.
26 of the loading process; correspondingly, the internal pressure drops 10-fold to a few atmospheres (ma
27 tion is presumed to be due to an increase in internal pressure due to optothermal heating of the CNTs
28  of the packaged genome on capsid structure, internal pressure, electrostatics and diffusion of water
29 ggests that the observed expansion is due to internal pressure exerted by the gaseous product in the
30                               Interestingly, internal pressure exerted by the maturing sarcomeres def
31 hedra in MH(6) phases is shown to arise from internal pressures exerted by large metal atoms, some of
32 levant items coalesced around three factors-'internal pressure', 'external pressure' and 'perceived c
33 olvent cohesion, such as surface tension and internal pressure, gave inferior correlations.
34  required stability needed to withstand high internal pressures generated upon genome loading and con
35 henomena where changes in cell stiffness and internal pressure have been implicated.
36 he inevitable result of gradually increasing internal pressure in a cylindrical cell.
37 rams, which was attributed to the release of internal pressure in bulk samples that disintegrated int
38                                         This internal pressure increases to ca. 1.9 GPa at the highes
39             We suggest that, on heating, the internal pressure increases, causing the DNA to exit-pro
40            When furrow ingression begins and internal pressure increases, the stores of membrane with
41 vantages of concave-shaped structures, where internal pressure induced compressive stress within the
42                                              Internal pressure induces the inflation of the structure
43 artificial infant stomach model simulated an internal pressure-inducing reflux event (five reflux eve
44 ternal osmotic pressures, which reveals that internal pressure is capable of powering ejection of the
45 ly hemifusion, but also complete fusion when internal pressure is introduced in the model.
46  pump water out of the cell, thereby keeping internal pressure low.
47 of plant vascular tissue formation with cell internal pressure monitoring, revealing a novel function
48 d length (n: 288, p < 0.001), along with the internal pressure (n: 288, p < 0.001), were the only pre
49 rafast heating, we could estimate an initial internal pressure of 2.5 to 3.5 kilobar in the high-dens
50 ing cuffs were evaluated for 24 hrs using an internal pressure of 30 cm H2O.
51                                     The vast internal pressure of an appressorium is very challenging
52 NA condensation experiments, we measured the internal pressure of DNA arrays as a function of the DNA
53 while maintaining stability against the high internal pressure of packaged DNA.
54 de the first experimental evidence of a high internal pressure of tens of atmospheres within a eukary
55                                              Internal pressure of the embryo and tissue elastic prope
56 y, the confinement is unyielding against the internal pressure of the microbombs, thereby enabling se
57 y, the solute dipolarity/polarizability, the internal pressure of water and the solubility parameter
58 ameters of carbon dioxide and water, and the internal pressure of water.
59 d together using this method could withstand internal pressures of >2250 psi, more than 1 order of ma
60 of oropharyngeal secretions simulant at cuff internal pressures of 15-30 cm H2O.
61 osquito proboscis dispense tip can withstand internal pressures of approximately 60 kPa, enabling eff
62 virus capsid; however, the in vivo effect of internal pressure on infection of bacteria is unknown.
63 e of the solution where the solute exerts an internal pressure on the boundary of the solution retain
64  of activation obtained using either solvent internal pressure or applied external pressure are very
65 eriments demonstrate that increasing solvent internal pressure or applied external pressure reduces t
66 olved in organic solvents with large solvent internal pressures ( partial differentialU/ partial diff
67 tial energy, entropy, free potential energy, internal pressure, pressure, and bulk modulus.
68     The high density of the genome exerts an internal pressure, requiring a maturation process that r
69 trachea contact area was determined using an internal pressure sensor within a tracheal model upon cu
70  After one viral genome is encapsidated, the internal pressure signals termination of packaging and e
71 hat cytoskeletal polymerization generates an internal pressure tending to keep cells convex, we find
72 ubes by using either diffusion or changes in internal pressure that are produced through body motion
73 s indicates that herpesviruses withstand the internal pressure that is generated during DNA genome pa
74 nstable because of a concomitant drop in the internal pressure, the drop caused by the metastability
75                             Below a critical internal pressure, the narrow ligaments between the void
76 e found that vasoconstriction in response to internal pressure-the vascular myogenic response-is blun
77 n the formation of cracks that evolve due to internal pressure; the expansion on the cracked surface
78                                       Use of internal pressure thereby provides unique insight into t
79                         Due to the increased internal pressure, these particles released a 3-fold lar
80 mers tied together by constraints exhibit an internal pressure; this idea is used to analyze physical
81 action during maturation may increase capsid internal pressure to trigger proper uncoating of adenovi
82 mp the DNA against the increasingly built-up internal pressure (up to 20 atm) in the capsid.
83 l capsids occurs under circumstances of high internal pressure, we also compute how much pressure a c
84 e induced by the QES, acting like a negative internal pressure, which drives the crystal into a "supe
85 s been developed to predict the shape of and internal pressure within the animal in response to a giv
86                                      Despite internal pressure within the safe range, transmitted tra
87 n vitro, the ejection depends sensitively on internal pressure within the virus capsid; however, the