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 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 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 assumption over paper that will help understand how our functions are mantic(p) to be stimulate during the expe! riment and thus be able to take away nigh data and some important initial and barrier conditions, incumbent for our model to work. From the Bobsbooms paper Passive transverse mechanical properties of penniless muscle in compression we are supposed to take the ramp and hold data (u versus t graph) and correspond 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 rent a full essay, order it on our website: BestEssayCheap.com
If you want to get a full essay, visit our page: cheap essay
No comments:
Post a Comment
Note: Only a member of this blog may post a comment.