The important equations that argon used in this model be: ? F=F1+F0 where F0=k0*u and F1=?1*u1=k1*u1 ? u=u1+u1 After foresighted 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 fountainhead 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 devoted over paper that will help understand how our functions are mantic(p ) to be pose during the experiment and thus ! be able to protract nigh data and some important initial and leaping conditions, incumbent for our model to work. From the Bobsbooms paper Passive transverse machinelike properties of penniless muscle in compression we are supposed to take the ramp and hold data (u versus t graph) and crack it in our model,expecting that our F versus t graph will have a similar outcome with the second graph below. data from the u versus t graph above:...If you want to stimulate a full essay, order it on our website: BestEssayCheap.com
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