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russs (0)

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a body is thrown from the surface of earth with an angle  to he horizontal.assuming the air drag to be negligible find the curvature radii of trajectory at its initial point and at its peak
    
ashish_banga (975)

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at the initial point it is u^2/ gcos alpha
at the peak =
u^2 cos^2 alpha / g
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me_living4u (56)

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at initial point....
velo. = u
and acc. radial.. centripetal= u^2/R
this acc. is provided by acc. due to grav. = gcos alpha (see acc. only perp. to vel.)
so gcos alpha = u^2/R
 
=> R= u^2/gcos alpha
 
similarly at topmost point
acc. due to grav=g
and vel. = ucos alpha
so R=  u^2cos^2 alpha/g
 
 
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iamtop1 (42)

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horizontal
ux= U Cos ?
motion along horizontal
x= Ux t +1/2 axt2
ax=0
x= U Cos ? t or t= x /U Cos ?

motion along vertical
y= Uy t + ½ ay t2

y= U sin ? t + ½ (-g) t2
= U sin ? t ? ½ g t2
Putting t = x/U Cos ?
y= U sin ? x/ U Cos ? - ½ g x2/U2 cos2 ?
tan ? - (g/2U2Cos2 ?) x2 called trajectory



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sarthak321 (62)

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A point undergoing any type of motion can assumed to be undergoing circular motion at any pt of its trajectory however the circles keep on changing with the position.

As we all know the  centripital acceleration of a body is given by 2R
or simply V2net/R (as R=V)

now at the highest pt of the trajectory the particle has net velocity in x direction

since in x we dont have any acceleration u remains constant and equal to ucos

now (ucos)2/R=g  (since centripital acceleration is perpendicular to Vnet and here g is perpendicular to ucos at highest point))

so R=(ucos)2/g
 

....
I hope u like the answer.....

as for the 1st part i.e initial veleocity take component of g perpendicular to u
and use it as R...

rate me if my answer helped




 

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