ライフサイエンスコーパス: shear modulus

1 in the solid state (i.e., displays a nonzero shear modulus).

2 und to make the dominant contribution to the shear modulus.

3 ng from 0.85 per cent to 1.2 per cent of the shear modulus.

4 ctional ligands, with no impact on the gel's shear modulus.

5 equency-dependent enhancement of the complex shear modulus.

6 on time, clot formation kinetics and maximum shear modulus.

7 d agreement with the experimentally measured shear modulus.

8 e with the appropriate bending stiffness and shear modulus.

9 y an increase of approximately 3-fold in the shear modulus.

10 t corneas were tested to measure full stroma shear modulus.

11 temperature-strain dependence of the solid's shear modulus.

12 sed an 18% reduction in the membrane elastic shear modulus.

13 In addition, the increase in shear modulus across the phase transition provides a pos

14 Benefiting from extremely high shear modulus and high ionic transference number, solid

15 The shear modulus and its pressure derivative are = 33.7 GPa

16 + theta(e)) and omega is the frequency, (ii) shear modulus and mean-squared displacement are inversel

17 lly validated closed form expression for the shear modulus and resonance frequency of a singly clampe

18 Psl was shown to elevate the layer's shear modulus and shear viscosity but had no effect on t

19 developed to predict the macroscopic elastic shear modulus and the area expansion modulus of the red

20 nsitivity of such materials increased as the shear modulus and the Flory-Huggins interaction paramete

21 rigidity transition signaled by a vanishing shear modulus and transverse sound speed.

22 During this process, we measured the shear modulus and viscosity of the phagosomal environmen

23 lation on its mechanical properties (elastic shear modulus and viscosity).

24 hanical properties (i.e., yield strength and shear modulus) and a unique characteristic structural le

25 vior, manifested in the slow decrease of the shear modulus, and accompanied by an increase in bead fl

26 cal properties, including aggregate modulus, shear modulus, and permeability, were calculated by inde

27 e, pressure, shear stress, bulk modulus, and shear modulus are all related to each other via scaling

28 inter-particle spacing and the reduction in shear modulus as a function of strain (the Payne effect)

29 ns--notably with regard to solvation--of the shear modulus behavior.

30 loy CGMD on a small RBC patch to compute the shear modulus, bending stiffness, and network parameters

31 eters (beta = 0.6, P < .001, R(2) = 0.33 for shear modulus; beta = 0.6, P < .001, R(2) = 0.32 for ela

32 3 cells has a strong influence on the cell's shear modulus but leaves its bulk modulus unchanged.

33 ect on the bulk modulus while increasing the shear modulus by approximately 6%, resulting in local an

34 e-sample measurements of the depth-dependent shear modulus, collagen fiber organization, and extracel

35 rize such a film: its thickness, density and shear modulus components (storage and loss moduli).

36 Shear modulus components extracted from these responses

37 coustically thick regime provide unambiguous shear modulus components.

38 thermodynamic parameters of iron, including shear modulus, compressional and shear velocities, heat

39 -to-one correspondence between toughness and shear modulus continuous over a broad range of inherent

40 We show that the shear modulus decreases from the cell center to the peri

41 ow firstly that the magnitude of the complex shear modulus decreases with progressive demyelination a

42 re pronounced, the step-like increase of the shear modulus diminishes and the Poisson's ratio becomes

43 The shear modulus from a 1% shear strain oscillatory test wa

44 The average shear modulus G = 55 Pa, which compares well with measur

45 The shear modulus G' determined from these measurements was

46 meterized by the frequency-dependent complex shear modulus G*(omega).

47 on line model of TSM resonators, the complex shear modulus (G' + jG'') and the average thickness (hPL

48 nning behavior and sufficiently high elastic shear modulus (G') to build self-supporting 3D structure

49 The classic linear relationship between shear modulus (G) and Vickers hardness (HV), along with

50 fluidic approach which allows measurement of shear modulus (G) during flow.

51 e (P) and temperature (T) derivatives of the shear modulus (G), namely ( partial differentialG/ parti

52 The absolute value of the complex shear modulus (|G*|) and the apparent diffusion coeffici

53 We find weak correlations between the shear modulus |G( *)| and both the collagen fiber orient

54 orders-of-magnitude increase in the complex shear modulus, G*, and formation of rigid hydrogels (G*

55 is calculated as a function of the in-plane shear modulus, H, and the out-of-plane bending modulus,

56 excitation allows this method to measure the shear modulus in a deeper specimen which extends the ela

57 state of actin filaments influences bulk and shear modulus in a similar manner.

58 s is seen most dramatically as a decrease in shear modulus in the neighborhood of the sensory hair ce

59 sults indicate that neutrophil viscosity and shear modulus increase by factors of 3.4, for 10(-9) M f

60 s G' and loss modulus G'', components of the shear modulus, increased approximately 33-fold and appro

61 ion, the frequency dependence of the complex shear modulus is a power law with slope one-half, indica

62 challenge the conventional wisdom that large shear modulus is a reliable predictor of hardness and st

63 The shear modulus is found proportional to the square root o

64 The local intracellular complex shear modulus is measured from the relaxation of the bea

65 Shear modulus is used as the representative parameter to

66 Our shear modulus microscopy can thus map the spatial distri

67 tetramer molecule and corresponding in-plane shear modulus mu(0) approximately 8.3 microN/m, our mode

68 sponse of the network is used to compute the shear modulus (mu) and area expansion modulus (kappa) fo

69 The shear-modulus-normalized CRSS of the HEA is not exceptio

70 elastic timescale of approximately 1 s and a shear modulus of approximately 1000 Pa.

71 reported discrepancy between the calculated shear modulus of postperovskite free aggregates and the

72 arge part be explained by an increase in the shear modulus of the (4)He solid identified by Day and B

73 the stall stress of actin gel growth and the shear modulus of the actin gel, actin polymerization can

74 rred to be proportional to the instantaneous shear modulus of the cell cortex, a parameters that we t

75 ustically thin films, changes in the complex shear modulus of the coatings contribute less than 5% of

76 The mean particle size, flow behaviour, and shear modulus of the materials depended on positive-to-n

77 reduced spectrin network connectivity on the shear modulus of the membrane.

78 e elastic property of the clots increase the shear modulus of the sample, altering the propagating ve

79 al regions and five radial zones and map the shear modulus of the TM using atomic force microscopy, a

80 Relatively low shear modulus of ~64 GPa from theoretical calculations s

81 ower-law dependence with exponent 3/2 of the shear modulus on stress, whereas the latter mechanism is

82 a characteristic power-law dependence of the shear modulus on the applied frequency.

83 ts the particle and spectrin the tether, the shear modulus predicted corresponds to the measured valu

84 was significantly higher when measuring the shear modulus rather than the apparent diffusion coeffic

85 3C and Al3BC3, their ideal shear strength to shear modulus ratios attain remarkably high values of 1.

86 with 23 wt% perfluoropolyether exhibits low shear modulus relative to neat glass electrolytes, ionic

87 s are expressed in terms of storage and loss shear modulus signatures, G'(E, T, omega) and G''(E, T,

88 es (where B is the bending modulus and H the shear modulus); taking the literature value of 2 x 10(-1

89 ansition is associated with softening of the shear modulus that could provide a significant seismic s

90 nt experiment found a marked increase in the shear modulus that shares the same temperature and heliu

91 of VIFs doubles the value of the cytoplasmic shear modulus to approximately 10 Pa.

92 opagation speed and by the ratio of material shear modulus to hydrodynamic pressure.

93 ation at finite packing is expected when the shear modulus vanishes.

94 ics to obtain analytical expressions for the shear modulus, viscosity, and fragility in terms of the

95 The local shear modulus was measured at various positions througho

96 approximately 5%, and no significant loss of shear modulus was noted.

97 arameter that can quantitatively predict the shear modulus, which is at the heart of many key propert

98 The significant variations in shear modulus with effective time scale can be "normaliz

99 All regions retained their shear modulus within 0.5% of instantaneous values when s

100 splacements imply decreases in the effective shear modulus within the kilometer-wide fault zones, ind