Question 57 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:

(x+y) dy+(x−y) dx=0;y=1 when x=1(x + y) \, dy + (x - y) \, dx = 0; \quad y = 1 \text{ when } x = 1
Correct Answer

The particular solution is:

tan⁡−1(yx)+12ln⁡(x2+y2)=π4+12ln⁡2\tan^{-1}\left(\frac{y}{x}\right) + \frac{1}{2}\ln(x^2 + y^2) = \frac{\pi}{4} + \frac{1}{2}\ln 2
Exercise: EXERCISE 9.4 | Q: 11 | (Page 22)
For More Understanding

Explanation

This is a homogeneous differential equation from Exercise 9.4. The equation can be rearranged to:

dydx=y−xx+y\frac{dy}{dx} = \frac{y-x}{x+y}

which is homogeneous since both numerator and denominator are homogeneous functions of degree 1. Using the substitution y=vxy = vx transforms it into a separable equation in vv and xx.

Solution Steps

  1. Step 1: Rewrite the equation as (x+y) dy=−(x−y) dx(x+y) \, dy = -(x-y) \, dx, giving:

    dydx=y−xx+y\frac{dy}{dx} = \frac{y-x}{x+y}

    This is a homogeneous differential equation.

  2. Step 2: Substitute y=vxy = vx, so dydx=v+xdvdx\frac{dy}{dx} = v + x\frac{dv}{dx}. The equation becomes:

    v+xdvdx=vx−xx+vx=v−1v+1v + x\frac{dv}{dx} = \frac{vx - x}{x + vx} = \frac{v-1}{v+1}
  3. Step 3: Simplify to get:

    xdvdx=v−1v+1−v=−1−v2v+1x\frac{dv}{dx} = \frac{v-1}{v+1} - v = \frac{-1-v^2}{v+1}

    which gives:

    v+1v2+1 dv=−dxx\frac{v+1}{v^2+1} \, dv = -\frac{dx}{x}
  4. Step 4: Integrate both sides:

    ∫v+1v2+1 dv=−∫dxx\int\frac{v+1}{v^2+1} \, dv = -\int\frac{dx}{x}

    This gives:

    tan⁡−1(v)+12ln⁡(v2+1)=−ln⁡∣x∣+C\tan^{-1}(v) + \frac{1}{2}\ln(v^2+1) = -\ln|x| + C
  5. Step 5: Substitute back v=yxv = \frac{y}{x}:

    tan⁡−1(yx)+12ln⁡(x2+y2x2)=−ln⁡∣x∣+C\tan^{-1}\left(\frac{y}{x}\right) + \frac{1}{2}\ln\left(\frac{x^2+y^2}{x^2}\right) = -\ln|x| + C

    Simplifying:

    tan⁡−1(yx)+12ln⁡(x2+y2)=C\tan^{-1}\left(\frac{y}{x}\right) + \frac{1}{2}\ln(x^2+y^2) = C
  6. Step 6: Apply the condition y=1y = 1 when x=1x = 1:

    tan⁡−1(1)+12ln⁡(2)=C\tan^{-1}(1) + \frac{1}{2}\ln(2) = C

    giving:

    C=π4+12ln⁡2C = \frac{\pi}{4} + \frac{1}{2}\ln 2