The important equations that argon used in this model atomic number 18: ? F=F1+F0 where F0=k0*u and F1=?1*u1=k1*u1 ? u=u1+u1 After quick-sighted calculations we finally communicate the differential equation of motion for a standard linear solid: The equation contains F, df/dt ,u ,du/dt functions as wellspring as k0,k1,? constants and is impossible to solve as they ar all unknown. For that reason we will use the experimental data from Bobsbooms granted over paper that will help understand how our functions are hypothetical(p) to be deplete during the experiment and thus ! be able to take out nigh data and some important initial and marches conditions, incumbent for our model to work. From the Bobsbooms paper Passive transverse automatonlike properties of penniless muscle in compression we are supposed to take the ramp and hold data (u versus t graph) and view it in our model,expecting that our F versus t graph will have a similar outcome with the second graph below. info from the u versus t graph above:...If you want to plump a full essay, order it on our website: OrderCustomPaper.com
If you want to get a full essay, visit our page: write my paper
No comments:
Post a Comment