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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 18:14:34 IST
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The rod AB is hinged at end A . If it is released from the horizontal position, then find the loss in gravitational potential energy at the instant when the acceleration of the end B has the magnitude 'g' .The mass of the rod is 'M' and the length is 'l'.
(a) Mgl/2
(b) 3Mgl/4
(c) 2Mgl/3
(d) Mgl/3
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:04:31 IST
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take any position of rod at an angle  . for calculating (Mg sin  )L/2=I  WHERE WE TAKE I ABOUT HINGE THUS I = ML^2/3 THUS  = (3gsin  )/2L AND APPLYING ENERGY CONSERVATION WE GET (MgL cos  )/2 = 1/2 I  ^2 THUS  ^2= (3g cos  )/L NOW NET ACCELERATION OF POINT B WILL BE =  [(a t)^2 +( a r)^2] a t =  L = [(3g sin  )/2L]L = (3 g sin  )/2 a r = (  ^2)L = 3 g cos  thus( A B) ^ 2 = 9g^2 cos ^ 2  + (9g ^2 sin ^ 2  ) /4...............1 g^2= the above equation but i m not getting the answer can u point the mistake? avery absurd answer is coming none from the options given
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:29:24 IST
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I also tried it this way...But I'm getting sin(theta)>1...
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:32:39 IST
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SOLVE THE LAST EQN WHICH I WROTE U WILL COS WHICH IS COMING VERY ABSURD PLZ JUST TRY IT OUT..
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:33:02 IST
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Well I think the acc. will be 'g' when the rod reaches the other end...
Since v=0 ,only a(tangential) = g is present
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:33:32 IST
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Well I think the acc. will be 'g' when the rod reaches the other end...
Since v=0 ,only a(tangential) = g is present
But then loss in GPE is zero
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:38:43 IST
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NO I DONT THINK SO BECAUSE THEN  = 3gL/2 THUS TANGENTIAL ACCN = 3g/2 of point B..
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:45:32 IST
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let angle made by rod with horizontal be x (Mg sin x)L/2=I  I is taken about hinge, I = ML 2 /3 THUS  = (3gsin x )/2L but a=r and a should be equal to g,implies =g/r equating, sinx =2/3 implies loss in PE is mg(l/2)sinx= 1/3mgl therefore D) I think I am right. That solves the problem!
<the missing pictures represent alpha(angular acceleration)>
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:54:12 IST
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well amaron even i m getting cos^2  negative which is not possible... so i think the situation will not come...when a = g
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:54:36 IST
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Well..I do not know enough abt differentiation coz I'm inXI th..
But are you really below Xth...?
what I really mean is that I don't get it
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:55:53 IST
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hey,look at my edited post! <I had made am mistake in my earlier post at a very early stage >
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:56:29 IST
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well neeraj did u get my method?
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 21:58:11 IST
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Hey...
In your Ist solution...mistake
You have taken total acc the vector sum of a(tan) and a(rad) but the total acceleration is given by A= L(alpha)
I'm getting sin(theta)= 2/3
Thus cos(theta) = root(5)/3
But again none of the options match
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 22:10:41 IST
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hey neeraj,I dont see the problem! if you have got sin(theta)=2/3 you have solved the problem as loss in PE is given by mglsin(theta) therefore ans can easily be got <I think its mgl/3 >
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 19 Feb 2007 22:11:05 IST
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