squareroot
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No.I'm really stuck with this one, i think I'm having the biggest mind block of my life so far. 


What value of x makes mgsin(α)-bxmgcos(α) = 0?squareroot said:No.I'm really stuck with this one, i think I'm having the biggest mind block of my life so far.![]()
No, you want to shift the origin of x by that much. I.e. instead of using x as the measure of displacement you use, say, u = x - tan(α)/b. The variable u should then satisfy the standard form for SHM.squareroot said:Well that would mean that mgsin(α)=bxmgcos(α) so do I write x=mgsin(α)/bmgcos(α) ?
All this has done is measure x from a different point on the plane. Or to put it another way, we found the equilibrium position, which was not x=0. It is u=0.squareroot said:and where woud I use this u?
You don't have to anything with it. Reformulating in terms of this u allows you to recognise the equation as being an exact fit for SHM. That allows you to figure out the frequency and amplitude in the usual way. Your problem was that extra constant term in the acceleration; rewriting it with u got rid of that.squareroot said:well yea, but what do i do with this u?
Because that is where the acceleration will be 0.and why is the equillibrium position at u=0?
The object starts at rest and we want the time until it is at rest again. Whether we measure distance as x or u does not affect the speed, so it's the time between successive points of zero speed in the SHM equation. How does that relate to the period of oscillation?squareroot said:Ok, so now i can say that k=-b*mgcos(β) so that period T=2π√(m/k), T=2π√(m/-bmgcos(β)) , T=2π√1/(-bgcos(β)) , and the frequency is 1/T.
But how do i get from this equations to those which help me find the actual distance and time that i need?