• A modification to the existing hardening function is proposed to reduce the mesh sensitivity of the plastic strain at peak stress.

    为了克服峰值塑性应变网格敏感性,对现有强化函数进行修正

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  • Plastic silicon rectifier. Max recurrent peak reverse voltage 1600 V. Max average forward rectified current 1.0 a.

    塑料整流经常性最大峰值反向电压1600,最大平均整流电流1.0A

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  • Research results:Residual strength of slip soil has linear regression with peak strength; plastic index can be better used to estimate residual strength.

    研究结果滑带峰值强度残余强度比较接近,成线性关系;塑性指数好的用来估算残余强度。

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  • Plastic silicon rectifier. Max recurrent peak reverse voltage 1300 V. Max average forward rectified current 1.0 A.

    塑料整流最大经常峰值反向电压为1300V最大平均正向整流电流1.0 A。

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  • Plastic silicon rectifier. Max recurrent peak reverse voltage 1250 V. Max average forward rectified current 1.0 A.

    塑料整流最大经常峰值反向电压为1250 V。最大平均正向整流电流1.0 A。

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  • Silicon rectifier. Case molded plastic. Maximum recurrent peak reverse voltage 1600 V. Maximum average forward rectified current 1.0 a.

    整流案例模压塑料经常性最大峰值反向电压1600,最大平均整流电流1.0A

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  • General purpose plastic rectifier. Maximum recurrent peak reverse voltage 1250 V. Maximum average forward rectified current 1.0 a.

    通用塑料整流器经常性最大峰值反向电压1250,最大平均整流电流1.0A

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  • Silicon rectifier. Case molded plastic. Maximum recurrent peak reverse voltage 1300 V. Maximum average forward rectified current 1.0 a.

    整流案例模压塑料经常性最大峰值反向电压1300V最大平均正向整流电流1.0 A。

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  • Fast switching plastic rectifier. Max recurrent peak reverse voltage 1000 V. Max average forward rectified current 1.0 a.

    快速开关塑料整流器最大经常峰值反向电压为1000V最大平均正向整流电流1.0 A。

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  • Plastic silicon rectifier. Max recurrent peak reverse voltage 400 V. Max average forward rectified current 1.0 A.

    塑料整流最大经常峰值反向电压为400 V,最大平均整流电流1.0A

    youdao

  • Plastic silicon rectifier. Max recurrent peak reverse voltage 100 V. Max average forward rectified current 1.0 A.

    塑料整流最大经常峰值反向电压为100V最大平均正向整流电流1.0 A。

    youdao

  • Silicon rectifier. Case molded plastic. Maximum recurrent peak reverse voltage 200 V. Maximum average forward rectified current 1.0 a.

    整流案例模压塑料经常性最大峰值反向电压200,最大平均整流电流1.0A

    youdao

  • Silicon rectifier. Case molded plastic. Maximum recurrent peak reverse voltage 400 V. Maximum average forward rectified current 1.0 a.

    整流案例模压塑料经常性最大峰值反向电压400V,最大平均整流电流1.0A

    youdao

  • Silicon rectifier. Case molded plastic. Maximum recurrent peak reverse voltage 100 V. Maximum average forward rectified current 1.0 A.

    整流案例模压塑料经常性最大峰值反向电压100V最大平均正向整流电流1.0 A。

    youdao

  • Silicon rectifier. Case molded plastic. Maximum recurrent peak reverse voltage 1000 V. Maximum average forward rectified current 1.0 A.

    整流案例模压塑料经常性最大峰值反向电压1000V最大平均正向整流电流1.0 A。

    youdao

  • General purpose plastic rectifier. Max recurrent peak reverse voltage 400 V. Max average forward rectified current 1.0 a.

    通用塑料整流器最大经常峰值反向电压为400 V,最大平均整流电流1.0A

    youdao

  • General purpose plastic rectifier. Max recurrent peak reverse voltage 200 V. Max average forward rectified current 1.0 a.

    通用塑料整流器经常性最大峰值反向电压200,最大平均正向整流电流1.0 A。

    youdao

  • General purpose plastic rectifier. Max recurrent peak reverse voltage 100 V. Max average forward rectified current 1.0 a.

    通用塑料整流器最大经常峰值反向电压为100V最大平均正向整流电流1.0 A。

    youdao

  • The rock strain softening after rock peak and the shear expansion properties affect the plastic critical state.

    岩石应变软化特性剪切膨胀特性塑性临界状态有重要影响

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  • The results indicate that particle breakage depends on the sample′s plastic work received during testing, and reduces the volume expansion and peak strength of the sands.

    结果表明颗粒破碎程度与输入的塑性密切相关;颗粒破碎的发生使钙质砂剪性减小,体积收缩应变增大,峰值强度降低

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  • Because of the rupture and plastic deformation, the altitude of the tiny peak had been decreased, so the surface roughness of the target back side improved.

    由于表面尖峰断裂塑性变形使尖峰高度降低因而表面质量得到提高。

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  • Fill with water, attach a plastic tube and pressure gauge and you're in business for motors with peak thrusts up to 140 LBS.

    填补附上塑料管压力业务汽车山顶主旨至140

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  • Firstly, dissipated energies induced by axial and lateral plastic deformations due to shear strain localization initiated at peak strength in strain softening stage is analyzed.

    首先由于应变软化阶段峰值强度剪切应变局部化启动纵向横向塑性变形引起耗散进行了分析。

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  • The results indicate that the peak values of compressive strength and the plastic deformation will increase significantly with the increment of the confining pressure.

    研究表明,复杂应力条件下,随着增大峰值抗压强度明显提高,塑性变形明显增大。

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  • The results indicate that the peak values of compressive strength and the plastic deformation will increase significantly with the increment of the confining pressure.

    研究表明,复杂应力条件下,随着增大峰值抗压强度明显提高,塑性变形明显增大。

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