Physics
6 Online
OpenStudy (anonymous):
Where should I start?
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OpenStudy (anonymous):
OpenStudy (anonymous):
centripetal force = tension
OpenStudy (anonymous):
ie mv^2/r=39 N
m*14*14/2.8=39
OpenStudy (anonymous):
m=39/70;
OpenStudy (anonymous):
I tried this answer; incorrect.
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OpenStudy (anonymous):
actually that's not right for a vertical path...
OpenStudy (anonymous):
decompose mg into radial and tangential components...
OpenStudy (anonymous):
you'll see that one component of mg provides some centripetal force...
so T will be less than mV^2/r
OpenStudy (anonymous):
Should I break the weight of the object into vertical and horizontal component? (x - direction is parallel to the direction of tension)
OpenStudy (anonymous):
not horizontal and vertical... for rotational problems the convenient axes are radial and tangential:
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OpenStudy (anonymous):
|dw:1350876752184:dw|
OpenStudy (anonymous):
|dw:1350876807379:dw|
OpenStudy (anonymous):
Isn't it the same as horizontal and vertical component?
OpenStudy (anonymous):
no.
OpenStudy (anonymous):
mg is vertical
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OpenStudy (anonymous):
If you let x direction be parallel to tension, then it is kind of the same thing.
OpenStudy (anonymous):
can u tel me is this correct @Algebraic! mg+mv^2/r=T
OpenStudy (anonymous):
@ashishthomas7 no..
OpenStudy (anonymous):
Like this:|dw:1350877052760:dw|
OpenStudy (anonymous):
@micahwood50 best to call it radial and tangential.... horizontal is something else entirely...
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OpenStudy (anonymous):
sure.
OpenStudy (anonymous):
I can't see the difference.
OpenStudy (anonymous):
or cut out the needless extra labels and just call it radial and tangential...
OpenStudy (anonymous):
since those are useful concepts in rotational motion...
OpenStudy (anonymous):
eg. V tangential = omega*r etc...
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OpenStudy (anonymous):
So \[\Large F_c = T + Wsin \theta = m a_c\]
OpenStudy (anonymous):
a radial = (V tangential)^2 /r and so on...
OpenStudy (anonymous):
Sorry, I don't know radial and tangential...
OpenStudy (anonymous):
just a components.