x=2sinθ−sin2θ ⇒ dθdx =
2cosθ−2cos2θ y=2cosθ−cos2θ ⇒ dθdy = –2sin
θ + 2sin2
θ dxdy=dθdxdθdy =
cosθ−cos2θsin2θ−sinθ This expression is simplified by recognizing that
sin2θ=2sinθcosθ and
cos2θ=2cos2θ−1 , leading to the expression:
dxdy=2sin2θ⋅sin23θ2sin2θ⋅cos23θ=cot23θ This is the rate of change of y with respect to x, as a function of θ.
Next, we differentiate this function with respect to θ to find
dx2d2y , yielding :
dx2d2y=dθd(dxdy)dxdθ=−23cosec223θ⋅dxdθ Here,
dxdθ is the reciprocal of
dθdx , so the equation becomes :
dx2d2y=2(cosθ−cos2θ)−23cosec223θ Finally, we evaluate this expression at
θ=π , yielding :
dx2d2y(π)=4(−1−1)−3=83 Therefore, the correct answer is (A)
83 .
Alternate Method : First, let's find the derivatives of x and y with respect to θ :
1)
dθdx=2cosθ−2cos2θ 2)
dθdy=−2sinθ+2sin2θ We know that
dxdy=dθdxdθdy So, we substitute 1) and 2) into this equation :
We have
dxdy=2cosθ−2cos2θ−2sinθ+2sin2θ=cosθ−cos2θsin2θ−sinθ For simplification, let's denote the numerator as
N=sin2θ−sinθ and the denominator as
D=cosθ−cos2θ .
We have to compute
dθd(dxdy) which is
dθd(DN) .
We can use the quotient rule for differentiation, which states that if we have a function of the form
vu , then its derivative is given by
v2vu′−uv′ .
So here,
N′=2cos2θ−cosθ and
D′=−sinθ+2sin2θ .
Applying the quotient rule :
dθd(dxdy)=D2DN′−ND′ Substituting the expressions for
N′ ,
D′ ,
N , and
D we get :
dθd(dxdy)=(cosθ−cos2θ)2(cosθ−cos2θ)(2cos2θ−cosθ)−(sin2θ−sinθ)(−sinθ+2sin2θ) Now
dx2d2y=dxd(dxdy)=dθd(dxdy)×dxdθ =
(cosθ−cos2θ)2(cosθ−cos2θ)(2cos2θ−cosθ)−(sin2θ−sinθ)(−sinθ+2sin2θ) ×(2cosθ−2cos2θ)1 ∴dx2d2yθ=πamp;=2(−1−1)3(−1−1)(2+1)−(0−0)(−0+0)amp;=−2×8−2×3=83