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2.7 Q-5

Question Statement

Given that

x=sin⁑θ,y=sin⁑(mθ),x = \sin \theta, \quad y = \sin(m \theta),

show that

(1βˆ’x2)y2βˆ’xy1+m2y=0.(1 - x^2) y_2 - x y_1 + m^2 y = 0.

Background and Explanation

This problem involves differentiating trigonometric functions. We are given expressions for xx and yy in terms of sin⁑θ\sin \theta, and the goal is to differentiate them to obtain a differential equation in terms of y1y_1 (the first derivative of yy with respect to xx) and y2y_2 (the second derivative of yy with respect to xx). To solve this, we need to use the chain rule for derivatives and some trigonometric identities.


Solution

Step 1: Express yy in terms of xx

We are given:

x=sin⁑θ⇒θ=sinβ‘βˆ’1(x)x = \sin \theta \quad \Rightarrow \quad \theta = \sin^{-1}(x)

and

y=sin⁑(mΞΈ)β‡’y=sin⁑(msinβ‘βˆ’1(x)).y = \sin(m \theta) \quad \Rightarrow \quad y = \sin(m \sin^{-1}(x)).

Step 2: Differentiate yy with respect to xx

To find y1y_1, differentiate both sides of y=sin⁑(msinβ‘βˆ’1(x))y = \sin(m \sin^{-1}(x)) with respect to xx using the chain rule:

dydx=ddx[sin⁑(msinβ‘βˆ’1(x))].\frac{dy}{dx} = \frac{d}{dx} \left[ \sin(m \sin^{-1}(x)) \right].

The derivative is:

y1=mcos⁑(msinβ‘βˆ’1(x))1βˆ’x2.y_1 = \frac{m \cos(m \sin^{-1}(x))}{\sqrt{1 - x^2}}.

Step 3: Multiply both sides by 1βˆ’x2\sqrt{1 - x^2}

This yields the expression for y1y_1 multiplied by 1βˆ’x2\sqrt{1 - x^2}:

(1βˆ’x2)y1=mcos⁑(msinβ‘βˆ’1(x)).\left( \sqrt{1 - x^2} \right) y_1 = m \cos(m \sin^{-1}(x)).

Step 4: Square both sides

To get a more manageable expression, square both sides:

(1βˆ’x2)y12=m2cos⁑2(msinβ‘βˆ’1(x)).(1 - x^2) y_1^2 = m^2 \cos^2(m \sin^{-1}(x)).

Step 5: Use the identity cos⁑2ΞΈ=1βˆ’sin⁑2ΞΈ\cos^2 \theta = 1 - \sin^2 \theta

Now, apply the trigonometric identity cos⁑2ΞΈ=1βˆ’sin⁑2ΞΈ\cos^2 \theta = 1 - \sin^2 \theta:

(1βˆ’x2)y12=m2(1βˆ’sin⁑2(msinβ‘βˆ’1(x))).(1 - x^2) y_1^2 = m^2 \left( 1 - \sin^2(m \sin^{-1}(x)) \right).

Step 6: Substitute y2=sin⁑2(msinβ‘βˆ’1(x))y^2 = \sin^2(m \sin^{-1}(x))

Since y=sin⁑(msinβ‘βˆ’1(x))y = \sin(m \sin^{-1}(x)), we know that y2=sin⁑2(msinβ‘βˆ’1(x))y^2 = \sin^2(m \sin^{-1}(x)), so we can substitute:

(1βˆ’x2)y12=m2(1βˆ’y2).(1 - x^2) y_1^2 = m^2 (1 - y^2).

Step 7: Differentiate again with respect to xx

Next, differentiate the entire equation with respect to xx to find y2y_2:

ddx[(1βˆ’x2)2y1y2βˆ’2xy12]=ddx[m2(βˆ’2yy1)].\frac{d}{dx} \left[ (1 - x^2) 2 y_1 y_2 - 2 x y_1^2 \right] = \frac{d}{dx} \left[ m^2 (-2y y_1) \right].

This simplifies to:

(1βˆ’x2)2y1y2βˆ’2xy12=βˆ’2m2yy1.(1 - x^2) 2 y_1 y_2 - 2x y_1^2 = -2 m^2 y y_1.

Step 8: Rearrange the terms

Now, rearrange the terms to isolate the desired equation:

(1βˆ’x2)y2βˆ’xy1+m2y=0.(1 - x^2) y_2 - x y_1 + m^2 y = 0.

Thus, we have proven that:

(1βˆ’x2)y2βˆ’xy1+m2y=0.(1 - x^2) y_2 - x y_1 + m^2 y = 0.

Key Formulas or Methods Used

  • Chain rule for derivatives: ddx[f(g(x))]=fβ€²(g(x))β‹…gβ€²(x)\frac{d}{dx} [f(g(x))] = f'(g(x)) \cdot g'(x)
  • Trigonometric identity: cos⁑2ΞΈ=1βˆ’sin⁑2ΞΈ\cos^2 \theta = 1 - \sin^2 \theta

Summary of Steps

  1. Express x=sin⁑θx = \sin \theta and y=sin⁑(mθ)y = \sin(m \theta).
  2. Differentiate y=sin⁑(msinβ‘βˆ’1(x))y = \sin(m \sin^{-1}(x)) with respect to xx using the chain rule to get y1y_1.
  3. Multiply both sides by 1βˆ’x2\sqrt{1 - x^2}.
  4. Square both sides to get (1βˆ’x2)y12=m2(1βˆ’y2)(1 - x^2) y_1^2 = m^2 (1 - y^2).
  5. Differentiate again with respect to xx to get the second derivative y2y_2.
  6. Rearrange the terms to show that (1βˆ’x2)y2βˆ’xy1+m2y=0(1 - x^2) y_2 - x y_1 + m^2 y = 0.