Question 59 of 96intermediate🔧 ApplyLong Answer4 marks

For each of the differential equations in Exercises from 11 to 15, find the particular solution satisfying the given condition:

[xsin⁡2(yx)−y]dx+xdy=0;y=π4 when x=1\left[x \sin^2\left(\frac{y}{x}\right) - y\right] dx + x dy = 0; \quad y = \frac{\pi}{4} \text{ when } x = 1
Correct Answer

cot(y/x) = ln|x| + 1

Exercise: EXERCISE 9.4 | Q: 13 | (Page 22)
For More Understanding

Explanation

This is a homogeneous differential equation. The equation can be rearranged to dydx=yx−sin⁡2(yx)\frac{dy}{dx} = \frac{y}{x} - \sin^2\left(\frac{y}{x}\right), which is a function of (yx)\left(\frac{y}{x}\right).

Using the substitution y=vxy = vx transforms it into a separable equation in terms of vv and xx. After integration and applying the boundary condition y=π4y = \frac{\pi}{4} when x=1x = 1, we get the particular solution.

Solution Steps

  1. Step 1: Rewrite the given differential equation.

    [xsin⁡2(yx)−y]dx+xdy=0\left[x \sin^2\left(\frac{y}{x}\right) - y\right] dx + x dy = 0 x dy=[y−xsin⁡2(yx)]dxx\, dy = \left[y - x \sin^2\left(\frac{y}{x}\right)\right] dx dydx=yx−sin⁡2(yx)\frac{dy}{dx} = \frac{y}{x} - \sin^2\left(\frac{y}{x}\right)
  2. Step 2: Identify that this is a homogeneous differential equation since the RHS is a function of (yx)\left(\frac{y}{x}\right).

    Substitute y=vxy = vx, so:

    dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}
  3. Step 3: Substitute and simplify.

    v+xdvdx=v−sin⁡2(v)v + x\frac{dv}{dx} = v - \sin^2(v) xdvdx=−sin⁡2(v)x\frac{dv}{dx} = -\sin^2(v) dvsin⁡2(v)=−dxx\frac{dv}{\sin^2(v)} = -\frac{dx}{x} cosec⁡2(v) dv=−dxx\cosec^2(v)\, dv = -\frac{dx}{x}
  4. Step 4: Integrate both sides.

    ∫cosec⁡2(v) dv=−∫dxx\int \cosec^2(v)\, dv = -\int \frac{dx}{x} −cot⁡(v)=−ln⁡∣x∣+C-\cot(v) = -\ln|x| + C cot⁡(v)=ln⁡∣x∣+C\cot(v) = \ln|x| + C
  5. Step 5: Replace v=yxv = \frac{y}{x} to get the general solution.

    cot⁡(yx)=ln⁡∣x∣+C\mathbf{\cot\left(\frac{y}{x}\right) = \ln|x| + C}
  6. Step 6: Apply the particular condition y=π4y = \frac{\pi}{4} when x=1x = 1.

    cot⁡(π4)=ln⁡∣1∣+C\cot\left(\frac{\pi}{4}\right) = \ln|1| + C 1=0+C1 = 0 + C C=1\mathbf{C = 1}
  7. Step 7: Write the particular solution.

    cot⁡(yx)=ln⁡∣x∣+1\mathbf{\cot\left(\frac{y}{x}\right) = \ln|x| + 1}