If x=2sinθ−sin2θ and y=2cosθ−cos2θ, θ∈[0,2π], then dx2d2y at θ = π is :
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Solution
x=2sinθ−sin2θ⇒dθdx = 2cosθ−2cos2θy=2cosθ−cos2θ⇒dθdy = –2sinθ + 2sin2θdxdy=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 = \frac{(\cos \theta - \cos 2\theta)(2\cos 2\theta - \cos \theta) - (\sin 2\theta - \sin \theta)(-\sin \theta + 2\sin 2\theta)}{(\cos \theta - \cos 2\theta)^2}$$$$ \times \frac{1}{(2 \cos \theta-2 \cos 2 \theta)} ∴dx2d2yθ=π=2(−1−1)3(−1−1)(2+1)−(0−0)(−0+0)=−2×8−2×3=83