ライフサイエンスコーパス: ductility

1 ercise in compromise between hardness versus ductility.

2 uch conflicting qualities as brittleness and ductility.

3 new avenues for improving their strength and ductility.

4 leness or an apparent loss of useful tensile ductility.

5 localization, resulting in near-zero tensile ductility.

6 with similar composition, yet, at identical ductility.

7 nergy, strengthen alloys without sacrificing ductility.

8 of metallic materials while preserving their ductility.

9 complements related studies of strength and ductility.

10 f crystalline materials such as strength and ductility.

11 rials, which often result in reduced surface ductility.

12 e expense of other important properties like ductility.

13 often interpreted as the reason for improved ductility.

14 g of the metastable phase produces increased ductility.

15 erials have high strength and relatively low ductility.

16 or by cold working with the expense of their ductility.

17 the future to design new alloys with higher ductility.

18 e material can be doubled at no reduction in ductility.

19 h or high strength but significantly reduced ductility.

20 ic glass heterostructures to achieve tensile ductility.

21 eld strength alloy without sacrificing alloy ductility.

22 nsile deformation, leading to a high tensile ductility--65% elongation to failure, and 30% uniform el

23 eels typically come at the expense of useful ductility, a dilemma known as strength-ductility trade-o

24 a strength of up to 2.2 gigapascals and good ductility (about 8.2 per cent).

25 l combination of ultrahigh strength and high ductility, along with increased strain-rate sensitivity.

26 tions in polycarbonate, a material with high ductility and a large Fracture Process Zone (FPZ).

27 ow substantial fracture toughness, they lack ductility and fail in an apparently brittle manner in un

28 differs greatly, leading to relatively poor ductility and formability.

29 al alloys which have significantly increased ductility and impact toughness, resulting from the ducti

30 strength to the caprock, contributing to its ductility and increased resistance to fracture.

31 well established even though they determine ductility and influence strengthening.

32 ribute, since an intrinsic lack of strength, ductility and low melting temperature severely restricts

33 ty of CTBs in strengthening, maintaining the ductility and minimizing the electron scattering is well

34 ng in Aluminium-5XXX alloys leads to reduced ductility and plastic instabilities at room temperature,

35 ic (FCC) structure is noteworthy because its ductility and strength increase with decreasing temperat

36 isplacive deformation mechanisms, maximizing ductility and strength simultaneously in nanoscale mater

37 or mechanical behaviors (high strength, high ductility and superelasticity) and novel physical proper

38 s physical insights into the origins of high ductility and superior reversibility of hybrid CNT struc

39 son's ratio and densification, connectivity, ductility and the toughness of solids; and their associa

40 fforded exceptional combination of strength, ductility and toughness for the nanofibrillar polymer co

41 m(1/2); at cryogenic temperatures strength, ductility and toughness of the CrCoNi alloy improve to s

42 one of the highest combinations of strength, ductility and toughness on record.

43 and compress, thereby enhancing the scale's ductility and toughness to prevent fracture.

44 serving as a continuous source of strength, ductility and toughness.

45 nstituent phases, and transformation-induced ductility and work-hardening capability are successfully

46 lectronic conductivity, mechanical adhesion, ductility, and electrolyte uptake.

47 with combinations of high strength, tensile ductility, and excellent fracture toughness.

48 The exceptional strength, ductility, and fatigue performance reported in this pape

49 deformation, affects fracture toughness and ductility, and is an important engineering material prop

50 to our understanding of plastic deformation, ductility, and mechanical strength of crystalline materi

51 f the polymer greatly improves the adhesion, ductility, and more importantly, the electrolyte uptake

52 he oxidation enhances the aluminium nanowire ductility, and the oxide shell exhibits superplastic beh

53 s of plastic deformation, strengthening, and ductility, and these complications pose significant chal

54 eneously with much lower strength but better ductility; and also show strengthening in tension but we

55 l) have large magnetostriction and excellent ductility; and they are very promising rare-earth free m

56 gth levels of approximately 1 GPa, excellent ductility ( approximately 60-70%) and exceptional fractu

57 Combinations of high strength and ductility are hard to attain in metals.

58 inite-element implementation, to predict the ductility as a function of temperature and strain rate i

59 crease in bone strength and increase in bone ductility associated with chronic inflammation and GC th

60 ing to their solubility in water and extreme ductility at raised temperatures (above approximately 12

61 e these excellent mechanical properties, low ductility at room temperature and poor microstructural s

62 ameters, predicts the observed steep drop in ductility at room temperature, which can be directly att

63 stalline materials often exhibit low tensile ductility at room temperature, which limits their practi

64 rare-earth intermetallic compounds with high ductility at room temperature.

65 s with excellent combination of strength and ductility, but also has great implications on overcoming

66 It is shown that the tension ductility can range from near zero percent to over ten p

67 taneously demonstrate high strength and high ductility, characteristics that are usually thought to b

68 Alloys with higher strength and ductility could alleviate some of these concerns by redu

69 Ductility-dip cracking in Ni-based superalloy, resulting

70 This combined increase in strength and ductility distinguishes the TRIP-DP-HEA alloy from other

71 However, they usually suffer from low ductility due to premature plastic instability by source

72 tical for metallic materials to achieve high ductility during plastic deformation.

73 the percolation theory that the compressive ductility, ec, can reach the maximum value at the interm

74 mechanical strength, while maintaining good ductility, electrical conductivity and thermal stability

75 ical heterogeneity, which offers a means for ductility enhancement, damage evolution and toughening.

76 BMG composites with room-temperature tensile ductility exceeding 10 per cent, yield strengths of 1.2-

77 base material, and the weld joint shows high ductility in bending which is accomplished through the o

78 As a commonly used method to enhance the ductility in bulk metallic glasses (BMGs), the introduct

79 rt the observation of an exceptional tensile ductility in crystalline copper/copper-zirconium glass n

80 listic penetrators, spacecraft shielding and ductility in high-performance ceramics.

81 etastable disorder or doping to achieve some ductility in intermetallic compounds at room temperature

82 means to enhance yield strength and tensile ductility in metals, nanotwinned metals generally fail w

83 anner, and observed a systematic increase in ductility in samples quenched under increasingly higher

84 te sensitivity and elucidating the origin of ductility in terms of the interactions of dislocations w

85 generates high strength, work hardening and ductility, including the easy motion of Shockley partial

86 spects provide guidance in designing tensile ductility into metallic glasses.

87 t is thought that one reason for the lack of ductility is that the development of - double twins (DTW

88 The increase in surface ductility is unexpected because it is the opposite patte

89 l mechanisms for increasing strength lead to ductility loss, an effect referred to as the strength-du

90 reminiscent of the "intermediate temperature ductility minimum" observed in polycrystalline metals.

91 occurs in unloading, which expounds the high ductility observed in the experiment.

92 tallic interfaces accounts for the extensive ductility observed.

93 The microstructure and tension ductility of a series of Ti-based bulk metallic glass ma

94 le strengths of approximately 1 GPa, tensile ductility of approximately 2-3 per cent, and an enhanced

95 and offers opportunities for controlling the ductility of BMG alloys.

96 material property that controls strength and ductility of crystals.

97 ides an easy and effective way to extend the ductility of intrinsically-brittle BMGs, opening up wide

98 Unfortunately, the ductility of magnesium alloys is usually limited.

99 which is very encouraging for improving the ductility of medium-carbon steels.

100 ome the inherent limitations in strength and ductility of Mg alloys.

101 We postulate that the ductility of nacre can be limited by eliminating tablet

102 We attribute the relatively high ductility of nano-twinned copper to the hardening of twi

103 f the microscopic structure underpinning the ductility of silica glass will not only pave the way tow

104 we develop a theory to quantify the kinetic ductility of single molecules from force spectroscopy ex

105 aterial properties associated with increased ductility of strut surfaces.

106 is probably related to temperature-dependent ductility of the crust at shallow depths (7 8 km on Euro

107 crimping explain the unexpected strength and ductility of the current BVS and point the way to thinne

108 ation, thus leading to enhanced strength and ductility of the TRIP-assisted dual-phase HEA engineered

109 C treatment in the TNF-Tg mice increased the ductility of tibiae under torsional loading.

110 In the present work, we show that the ductility of Zr-based BMGs with nearly zero plasticity i

111 ably an increased yield stress and decreased ductility, often accompanied by plastic flow localizatio

112 l materials requiring both high strength and ductility, properties that are often mutually exclusive.

113 bility is limited by their near-zero tensile ductility resulting from work-softening and shear locali

114 t twin structure can cause strengthening and ductility retention, and how sequential torsion and tens

115 excellent properties such as stretchability, ductility, shear-thinning, and thixotropy.

116 In particular, their poor ductility significantly impedes their industrial applica

117 0 times as that of single crystals, and with ductility simultaneously.

118 a combination of yield strength and tensile ductility that surpasses that of conventional 316L steel

119 he possible means of optimizing strength and ductility through interfacial engineering.

120 fabricate steels with high strength and high ductility (toughness).

121 s of mechanical properties such as strength, ductility, toughness, elasticity and requirements for pr

122 To understand how the strength-ductility trade-off can be defeated, we apply in situ, a

123 The strength-ductility trade-off has been a long-standing dilemma in

124 It is shown that this evasion of strength-ductility trade-off is due to the formation of a gradien

125 have attempted to evade this strength versus ductility trade-off, but the paradox persists.

126 seful ductility, a dilemma known as strength-ductility trade-off.

127 loss, an effect referred to as the strength-ductility trade-off.

128 h of twinning-induced plasticity steel at no ductility trade-off.

129 ons on overcoming the long-standing strength-ductility tradeoff of metallic materials in general.

130 hows that the trade-off between strength and ductility typically observed for metallic materials is s

131 Remarkable tensile ductility was first obtained in an in-situ Ti-based bulk

132 only provide strength but also contribute to ductility, which is very encouraging for improving the d

133 sought goal in metallic glasses is to impart ductility without conceding their strength and elastic l