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 farseeing 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 be all unknown. For that reason we will use the experimental data from Bobsbooms given(p) over paper that will help understand how our functions are divinatory(p) to be cons truct during the experiment and thus be ! able to move out nigh data and some important initial and limit point conditions, incumbent for our model to work. From the Bobsbooms paper Passive transverse mechanistic properties of penniless muscle in compression we are supposed to take the ramp and hold data (u versus t graph) and oppose it in our model,expecting that our F versus t graph will have a similar outcome with the second graph below. information from the u versus t graph above:...If you want to locomote a full essay, order it on our website: BestEssayCheap.com
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