1
Hodge Conjecture
·2010-08-11 11:57:36
no.....
ans. is = mm+M H cot( theta)
1
Euclid
·2010-08-11 17:42:31
The wedge moves only due to the sine component of N provided by the block...
assume that the accn of wedge is 'a'(right) and that of block is 'b' (down the plane wrt wedge)
Now find out the absolute accn of block if u solve from ground frame..or add a pseudo force if u solve wrt wedge.
30
Ashish Kothari
·2010-08-12 09:12:49
Let \: a_{0}\: be \: the \: acc.\: of \: the \: block.
Let \: a\: be \: the \: acc.\: of \: the \: wedge.
Therefore,
ma_{0}= \: mgsin\theta \: + macos\theta \:....(1)
N=mgcos\theta \: - \:masin\theta \: ..... \:(2)
Nsin\theta = Ma \: .... (3)
Solving 2 and 3,
a = \frac{mgsin\theta cos\theta }{M + msin^{2}\theta }
Using this to solve 1,
a_{0}= \frac{gsin\theta (M+m)}{M+msin^{2}\theta }
Now, the length of the inclined part = \frac{H}{sin\theta }
Hence, displacement of block,
\frac{H}{sin\theta } = \frac{1}{2}\frac{gsin\theta (M+m) }{(M + msin^{2}\theta )} t^{2}
\Rightarrow t^{2} = \frac{2H(M+msin^{2}\theta )}{gsin^{2}\theta (M+m)}
Therefore, distance travelled by wedge,
D = \frac{1}{2}\frac{mgsin\theta cos\theta}{(M+msin^{2}\theta)}t^{2}
D = \frac{m}{M+m}Hcot\theta [Ans.]
30
Ashish Kothari
·2010-08-12 09:26:29
:)
I hope this will help a little more.
The FBDs of the wedge and the block.
1
Hodge Conjecture
·2010-08-12 10:05:38
@ ashish_k04.....thnx for posting diagram....but to be honest there wasn't any need for that.....i too did d same thing but made calculation mistake in calculating a :) ............
but this problem is really good example to show how powerful center of mass concept is.......using COM just a single eq. will give the desired result.................