a pendulum of mass m and length L is pulled back an angle θ and released. After the pendulum swings through its lowest point, it encounters a peg α degrees out and r meters from the top of the string. The mass swings up about the peg until the string becomes slack with the mass falling inward and hitting the peg. show that cosθ=r/Lcosα-√3/2(1-r/L)
I tried to find the forces on the pendulum at the initial and final position Lcosθ-mg=0 Lsinθ=ma rcosθ-mg=0 rsinθ=ma but it doesn't seem to work at all. what I get is that r=L which is impossible. :(
noyhing
pellet man i am stuck....!!
pellet man
pellet means what
Dude how can i get it solved?
one minute i am thinking solution
hey aryan are you listening
yeah i am here...
see take cos and tan make them negative of pendulum opposite position and make it positive and you will find your answer ok got it so easy
ok got it aryan
ok i will try..if i am stuck i will get back to you.
ok np
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