A particle
is initially at a distance of
from point
. The particle
moves with a velocity given by
where
is a unit vector from
to
at any time t.
Initially is perpendicular to .
Find the time in second after which point meets point .
Details and Assumptions:
is unit vector along the direction of x-axis.
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Even though not stated, O can be taken to be the origin without any loss of generality. The initial position of P can be taken as ( 0 , 1 6 ) . (It can also be taken as ( 0 , − 1 6 ) , both of which will give the same answer.)
Let the position of the point at any time t be r = x i ^ + y j ^ . This gives that P O = − x i ^ − y j ^ and the unit vector will be − x 2 + y 2 x i ^ − x 2 + y 2 y j ^ .
∴ v = 5 ( − x 2 + y 2 x i ^ − x 2 + y 2 y j ^ ) + 3 i ^
⟹ v = ( x 2 + y 2 − 5 x + 3 ) i ^ + ( x 2 + y 2 − 5 y ) j ^
Using the definition of velocity, v = d t d x i ^ + d t d y j ^
d t d x = x 2 + y 2 − 5 x + 3 ( 1 )
d t d y = x 2 + y 2 − 5 y ( 2 )
Diving ( 1 ) by ( 2 ) :
d y d x = 5 y 5 x − 3 x 2 + y 2 = y x − 5 3 1 + ( y x ) 2
Using the substitution: x = u y ⟹ d y d x = u + y d y d u :
u + y d y d u = u − 5 3 1 + u 2
⟹ 1 + u 2 d u = − 5 3 y d y
Integrating both sides:
ln ( 1 + u 2 + u ) = − 5 3 ln ( y ) + C
Using initial conditition of x = 0 when y = 1 6 , C can be found to be equal to 5 3 ln ( 1 6 )
∴ ln ( 1 + u 2 + u ) = − 5 3 ln ( 1 6 y )
Taking anti-log:
1 + u 2 + u = ( 1 6 y ) − 5 3 ( 3 )
1 + u 2 − u = ( 1 6 y ) 5 3 ( 4 ) ( Using the fact that ( 1 + u 2 + u ) ( 1 + u 2 − u ) = 1
Adding the two:
1 + u 2 = 2 1 [ ( 1 6 y ) − 5 3 + ( 1 6 y ) 5 3 ]
⟹ y x 2 + y 2 = 2 1 [ ( 1 6 y ) − 5 3 + ( 1 6 y ) 5 3 ]
Subsituting the above in ( 2 ) :
2 1 [ ( 1 6 y ) − 5 3 + ( 1 6 y ) 5 3 ] = − 5 d y d t
⟹ 2 1 ∫ 1 6 0 [ ( 1 6 y ) − 5 3 + ( 1 6 y ) 5 3 ] d y = − 5 ∫ 0 T d t
⟹ 2 1 [ 1 6 5 2 1 ( 1 6 y ) 5 2 + 1 6 5 8 1 ( 1 6 y ) 5 8 ] 1 6 0 = − 5 T
⟹ 2 5 [ 1 6 2 1 ( − 1 ) + 1 6 8 1 ( − 1 ) ] = − 5 T
⟹ T = 5