User contributions for 129.13.0.0/16

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22:2422:24, 5 January 2015 diff hist +580 Jacobi elliptic functions 129.13.72.196 talk →Definition as trigonometryhttp://www.und.edu/instruct/schwalm/MAA_Presentation_10-02/handout.pdf current

11:2811:28, 30 December 2014 diff hist +91 Supercontinuum 129.13.244.211 talk →The 1960s and 1970s current

13:0713:07, 17 December 2014 diff hist −124 Brent–Kung adder 129.13.186.4 talk less performance: means higher gate delay count in this case current

18:4618:46, 20 November 2014 diff hist −2 Dehn function 129.13.72.197 talk →Growth types of functions: typo current

14:1314:13, 10 October 2014 diff hist +3 Uniform boundedness 129.13.72.197 talk →Real line and complex plane current

16:4416:44, 8 October 2014 diff hist +6 Power-law fluid 129.13.72.195 talk →Dilatant fluids: fluids don´t care about absolute deformation current
08:5508:55, 8 October 2014 diff hist +48 Weissenberg number 129.13.72.195 talk explain symbols. but isn´t relaxation time usually \tau, not \lambda ? current

11:1611:16, 29 April 2014 diff hist +273 Hu Washizu principle 129.13.72.198 talk No edit summary current

13:3913:39, 27 February 2014 diff hist +9 Extensional viscosity 129.13.72.198 talk No edit summary

16:2016:20, 13 November 2013 diff hist +1,941 N Momentum compaction 129.13.108.115 talk third definition of α

14:0214:02, 7 October 2013 diff hist +18,787 N DEVS 129.13.72.198 talk →Other Formalisms

11:2811:28, 4 September 2013 diff hist +3,215 N Stress relaxation 129.13.72.198 talk Maxwell and Voigt are the simplest models for liquids and solids respectively. the slsm is a rather simple derivative of a voigt model, and surely not "most accurate".

10:2810:28, 3 August 2012 diff hist +13,902 N Arruda–Boyce model 129.13.114.23 talk →Alternative expressions for the Arruda–Boyce model

16:0816:08, 25 April 2012 diff hist +4,073 N Pyrgeometer 129.13.72.198 talk →Measurement of long wave downward radiation

10:3710:37, 14 March 2012 diff hist +11,326 N Clutter (radar) 129.13.72.198 talk No edit summary

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