GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5

Get the most accurate GSEB Solutions for Class 12 Mathematics Chapter 09 Differential Equations here. Updated for the 2026-27 academic session, these solutions are based on the latest GSEB textbooks for Class 12 Mathematics. Our expert-created answers for Class 12 Mathematics are available for free download in PDF format.

Detailed Chapter 09 Differential Equations GSEB Solutions for Class 12 Mathematics

For Class 12 students, solving GSEB textbook questions is the most effective way to build a strong conceptual foundation. Our Class 12 Mathematics solutions follow a detailed, step-by-step approach to ensure you understand the logic behind every answer. Practicing these Chapter 09 Differential Equations solutions will improve your exam performance.

Class 12 Mathematics Chapter 09 Differential Equations GSEB Solutions PDF

In each of the questions 1 to 10, show that the given differential equation is homogeneous and solve each of them:

 

Question 1. \( (x^2 + xy) dy = (x^2 + y^2)dx \)
Answer: First, we can rewrite the given differential equation in the form \( \frac{dy}{dx} \):
\( \frac{dy}{dx} = \frac{x^2 + y^2}{x^2 + xy} = f(x, y) \) (let's call this equation (1))
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{(\lambda x)^2 + (\lambda y)^2}{(\lambda x)^2 + (\lambda x)(\lambda y)} \)
\( = \frac{\lambda^2 x^2 + \lambda^2 y^2}{\lambda^2 x^2 + \lambda^2 xy} \)
\( = \frac{\lambda^2 (x^2 + y^2)}{\lambda^2 (x^2 + xy)} \)
\( = \lambda^0 \left(\frac{x^2 + y^2}{x^2 + xy}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
Now, to solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into equation (1):
\( v + x \frac{dv}{dx} = \frac{x^2 + (vx)^2}{x^2 + x(vx)} \)
\( v + x \frac{dv}{dx} = \frac{x^2 + v^2 x^2}{x^2 + vx^2} \)
\( v + x \frac{dv}{dx} = \frac{x^2(1 + v^2)}{x^2(1 + v)} \)
\( v + x \frac{dv}{dx} = \frac{1 + v^2}{1 + v} \)
Now, we separate the variables:
\( x \frac{dv}{dx} = \frac{1 + v^2}{1 + v} - v \)
\( x \frac{dv}{dx} = \frac{1 + v^2 - v(1 + v)}{1 + v} \)
\( x \frac{dv}{dx} = \frac{1 + v^2 - v - v^2}{1 + v} \)
\( x \frac{dv}{dx} = \frac{1 - v}{1 + v} \)
\( \frac{1 + v}{1 - v} dv = \frac{dx}{x} \)
Now, integrate both sides:
\( \int \frac{1 + v}{1 - v} dv = \int \frac{dx}{x} \)
We can rewrite the left side as \( \int \frac{2 - (1 - v)}{1 - v} dv = \int \left(\frac{2}{1 - v} - 1\right) dv \):
\( \int \left(\frac{2}{1 - v} - 1\right) dv = \int \frac{dx}{x} \)
\( 2 \int \frac{1}{1 - v} dv - \int 1 dv = \int \frac{1}{x} dx \)
\( 2(-\log|1 - v|) - v = \log|x| + \log C \)
\( -2 \log|1 - v| - v = \log|x| + \log C \)
Now, substitute back \( v = \frac{y}{x} \):
\( -2 \log\left|1 - \frac{y}{x}\right| - \frac{y}{x} = \log|x| + \log C \)
\( -2 \log\left|\frac{x - y}{x}\right| - \frac{y}{x} = \log|x| + \log C \)
\( -2 (\log|x - y| - \log|x|) - \frac{y}{x} = \log|x| + \log C \)
\( -2 \log|x - y| + 2 \log|x| - \frac{y}{x} = \log|x| + \log C \)
Rearrange the terms:
\( \log|x| - 2 \log|x - y| - \frac{y}{x} = \log C \)
\( \log\left|\frac{x}{(x - y)^2}\right| - \frac{y}{x} = \log C \)
\( \log\left|\frac{x}{(x - y)^2}\right| = \frac{y}{x} + \log C \)
To eliminate the logarithm, we use exponential function:
\( \frac{x}{(x - y)^2} = e^{\frac{y}{x} + \log C} \)
\( \frac{x}{(x - y)^2} = e^{\frac{y}{x}} e^{\log C} \)
Let \( e^{\log C} = K \) (a new constant).
\( \frac{x}{(x - y)^2} = K e^{\frac{y}{x}} \)
\( (x - y)^2 = \frac{x}{K} e^{-\frac{y}{x}} \)
Let \( \frac{1}{K} = C_1 \) (another constant).
\( (x - y)^2 = C_1 x e^{-\frac{y}{x}} \)
This is the general solution.

In simple words: First, we checked if the equation was "homogeneous" by substituting \( \lambda x \) and \( \lambda y \). Since it was, we used a special trick: we replaced \( y \) with \( vx \) and \( \frac{dy}{dx} \) with \( v + x \frac{dv}{dx} \). This allowed us to separate the parts with \( v \) and \( x \) and then integrate both sides. Finally, we put \( \frac{y}{x} \) back for \( v \) to get the final answer.

Exam Tip: Remember to always first check for homogeneity. If it's homogeneous, the substitution \( y=vx \) is key, as it transforms the differential equation into a separable form that is easier to integrate.

 

Question 2. \( y' = \frac{x+y}{x} \)
Answer: We have the given differential equation \( y' = \frac{x+y}{x} \).
This can be written as \( \frac{dy}{dx} = \frac{x+y}{x} = f(x, y) \).
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{\lambda x + \lambda y}{\lambda x} \)
\( = \frac{\lambda(x+y)}{\lambda x} \)
\( = \lambda^0 \left(\frac{x+y}{x}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into the equation:
\( v + x \frac{dv}{dx} = \frac{x + vx}{x} \)
\( v + x \frac{dv}{dx} = \frac{x(1 + v)}{x} \)
\( v + x \frac{dv}{dx} = 1 + v \)
Now, separate the variables:
\( x \frac{dv}{dx} = 1 + v - v \)
\( x \frac{dv}{dx} = 1 \)
\( dv = \frac{dx}{x} \)
Now, integrate both sides:
\( \int dv = \int \frac{dx}{x} \)
\( v = \log|x| + C \)
Substitute back \( v = \frac{y}{x} \):
\( \frac{y}{x} = \log|x| + C \)
Multiply by \( x \) to get the final solution:
\( y = x \log|x| + Cx \)

In simple words: We first checked if the equation was homogeneous, which it was. Then, we replaced \( y \) with \( vx \) and \( y' \) with \( v + x \frac{dv}{dx} \). After simplifying, we separated the \( v \) and \( x \) terms and integrated them. Finally, we put \( \frac{y}{x} \) back for \( v \) to find the answer.

Exam Tip: For simple homogeneous equations like this, the substitution \( y=vx \) often leads to a direct integration. Be careful with constant of integration, often denoted as \( C \).

 

Question 3. \( (x - y)dy - (x + y)dx = 0 \)
Answer: We have the given differential equation \( (x - y)dy - (x + y)dx = 0 \).
We can rewrite this in the form \( \frac{dy}{dx} \):
\( (x - y)dy = (x + y)dx \)
\( \frac{dy}{dx} = \frac{x + y}{x - y} = f(x, y) \)
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{\lambda x + \lambda y}{\lambda x - \lambda y} \)
\( = \frac{\lambda(x + y)}{\lambda(x - y)} \)
\( = \lambda^0 \left(\frac{x + y}{x - y}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into the equation:
\( v + x \frac{dv}{dx} = \frac{x + vx}{x - vx} \)
\( v + x \frac{dv}{dx} = \frac{x(1 + v)}{x(1 - v)} \)
\( v + x \frac{dv}{dx} = \frac{1 + v}{1 - v} \)
Now, separate the variables:
\( x \frac{dv}{dx} = \frac{1 + v}{1 - v} - v \)
\( x \frac{dv}{dx} = \frac{1 + v - v(1 - v)}{1 - v} \)
\( x \frac{dv}{dx} = \frac{1 + v - v + v^2}{1 - v} \)
\( x \frac{dv}{dx} = \frac{1 + v^2}{1 - v} \)
\( \frac{1 - v}{1 + v^2} dv = \frac{dx}{x} \)
Now, integrate both sides:
\( \int \frac{1 - v}{1 + v^2} dv = \int \frac{dx}{x} \)
We can split the integral on the left side:
\( \int \frac{1}{1 + v^2} dv - \int \frac{v}{1 + v^2} dv = \int \frac{1}{x} dx \)
\( \tan^{-1} v - \frac{1}{2} \int \frac{2v}{1 + v^2} dv = \int \frac{1}{x} dx \)
\( \tan^{-1} v - \frac{1}{2} \log|1 + v^2| = \log|x| + C \)
Substitute back \( v = \frac{y}{x} \):
\( \tan^{-1}\left(\frac{y}{x}\right) - \frac{1}{2} \log\left|1 + \left(\frac{y}{x}\right)^2\right| = \log|x| + C \)
\( \tan^{-1}\left(\frac{y}{x}\right) - \frac{1}{2} \log\left|\frac{x^2 + y^2}{x^2}\right| = \log|x| + C \)
\( \tan^{-1}\left(\frac{y}{x}\right) - \frac{1}{2} (\log|x^2 + y^2| - \log|x^2|) = \log|x| + C \)
\( \tan^{-1}\left(\frac{y}{x}\right) - \frac{1}{2} \log|x^2 + y^2| + \frac{1}{2} \log|x^2| = \log|x| + C \)
\( \tan^{-1}\left(\frac{y}{x}\right) - \frac{1}{2} \log(x^2 + y^2) + \frac{1}{2} (2 \log|x|) = \log|x| + C \)
\( \tan^{-1}\left(\frac{y}{x}\right) - \frac{1}{2} \log(x^2 + y^2) + \log|x| = \log|x| + C \)
\( \tan^{-1}\left(\frac{y}{x}\right) - \frac{1}{2} \log(x^2 + y^2) = C \)
This is the general solution.

In simple words: We changed the given equation into the standard \( \frac{dy}{dx} \) form. We confirmed it was homogeneous by using \( \lambda x \) and \( \lambda y \). Then, we substituted \( y = vx \) to simplify, separated the \( v \) and \( x \) terms, and integrated each side. Finally, we put \( \frac{y}{x} \) back for \( v \) to get the solution.

Exam Tip: When integrating expressions involving \( \frac{v}{1+v^2} \), remember the form \( \int \frac{f'(x)}{f(x)} dx = \log|f(x)| + C \). Also, carefully handle the properties of logarithms during simplification, especially when dealing with \( \log|x^2| \).

 

Question 4. \( (x^2 - y^2)dx + 2xy dy = 0 \)
Answer: We have the given differential equation \( (x^2 - y^2)dx + 2xy dy = 0 \).
We can rewrite this in the form \( \frac{dy}{dx} \):
\( 2xy dy = -(x^2 - y^2)dx \)
\( 2xy dy = (y^2 - x^2)dx \)
\( \frac{dy}{dx} = \frac{y^2 - x^2}{2xy} = f(x, y) \)
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{(\lambda y)^2 - (\lambda x)^2}{2(\lambda x)(\lambda y)} \)
\( = \frac{\lambda^2 y^2 - \lambda^2 x^2}{2\lambda^2 xy} \)
\( = \frac{\lambda^2 (y^2 - x^2)}{\lambda^2 (2xy)} \)
\( = \lambda^0 \left(\frac{y^2 - x^2}{2xy}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into the equation:
\( v + x \frac{dv}{dx} = \frac{(vx)^2 - x^2}{2x(vx)} \)
\( v + x \frac{dv}{dx} = \frac{v^2 x^2 - x^2}{2vx^2} \)
\( v + x \frac{dv}{dx} = \frac{x^2(v^2 - 1)}{x^2(2v)} \)
\( v + x \frac{dv}{dx} = \frac{v^2 - 1}{2v} \)
Now, separate the variables:
\( x \frac{dv}{dx} = \frac{v^2 - 1}{2v} - v \)
\( x \frac{dv}{dx} = \frac{v^2 - 1 - 2v^2}{2v} \)
\( x \frac{dv}{dx} = \frac{-v^2 - 1}{2v} \)
\( x \frac{dv}{dx} = -\frac{v^2 + 1}{2v} \)
\( \frac{2v}{v^2 + 1} dv = -\frac{dx}{x} \)
Now, integrate both sides:
\( \int \frac{2v}{v^2 + 1} dv = -\int \frac{1}{x} dx \)
\( \log|v^2 + 1| = -\log|x| + \log C \)
\( \log(v^2 + 1) = \log\left|\frac{C}{x}\right| \)
\( v^2 + 1 = \frac{C}{x} \)
Substitute back \( v = \frac{y}{x} \):
\( \left(\frac{y}{x}\right)^2 + 1 = \frac{C}{x} \)
\( \frac{y^2}{x^2} + 1 = \frac{C}{x} \)
\( \frac{y^2 + x^2}{x^2} = \frac{C}{x} \)
Multiply by \( x^2 \):
\( y^2 + x^2 = Cx \)
This is the general solution.

In simple words: First, we rearranged the equation to get \( \frac{dy}{dx} \). We checked that it was homogeneous by substituting \( \lambda x \) and \( \lambda y \). Then, we used the substitution \( y = vx \) to make the equation simpler. After separating the terms with \( v \) and \( x \), we integrated both sides. Finally, we replaced \( v \) with \( \frac{y}{x} \) to find the overall answer.

Exam Tip: Pay close attention to the algebraic manipulation when separating variables, especially sign changes. The integral \( \int \frac{2v}{v^2+1} dv \) is a common pattern that results in a logarithm, so recognize this quickly.

 

Question 5. \( x^2 \frac{dy}{dx} = x^2 - 2y^2 + xy \)
Answer: We have the given differential equation \( x^2 \frac{dy}{dx} = x^2 - 2y^2 + xy \).
We can rewrite this in the form \( \frac{dy}{dx} \):
\( \frac{dy}{dx} = \frac{x^2 - 2y^2 + xy}{x^2} = f(x, y) \)
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{(\lambda x)^2 - 2(\lambda y)^2 + (\lambda x)(\lambda y)}{(\lambda x)^2} \)
\( = \frac{\lambda^2 x^2 - 2\lambda^2 y^2 + \lambda^2 xy}{\lambda^2 x^2} \)
\( = \frac{\lambda^2 (x^2 - 2y^2 + xy)}{\lambda^2 x^2} \)
\( = \lambda^0 \left(\frac{x^2 - 2y^2 + xy}{x^2}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into the equation:
\( v + x \frac{dv}{dx} = \frac{x^2 - 2(vx)^2 + x(vx)}{x^2} \)
\( v + x \frac{dv}{dx} = \frac{x^2 - 2v^2 x^2 + vx^2}{x^2} \)
\( v + x \frac{dv}{dx} = \frac{x^2(1 - 2v^2 + v)}{x^2} \)
\( v + x \frac{dv}{dx} = 1 - 2v^2 + v \)
Now, separate the variables:
\( x \frac{dv}{dx} = 1 - 2v^2 + v - v \)
\( x \frac{dv}{dx} = 1 - 2v^2 \)
\( \frac{dv}{1 - 2v^2} = \frac{dx}{x} \)
Now, integrate both sides:
\( \int \frac{dv}{1 - 2v^2} = \int \frac{dx}{x} \)
We can factor out \( 2 \) from the denominator:
\( \int \frac{dv}{2\left(\frac{1}{2} - v^2\right)} = \int \frac{dx}{x} \)
\( \frac{1}{2} \int \frac{dv}{\left(\frac{1}{\sqrt{2}}\right)^2 - v^2} = \int \frac{dx}{x} \)
Using the standard integral formula \( \int \frac{1}{a^2 - x^2} dx = \frac{1}{2a} \log\left|\frac{a + x}{a - x}\right| \), where \( a = \frac{1}{\sqrt{2}} \):
\( \frac{1}{2} \left[\frac{1}{2 \cdot \frac{1}{\sqrt{2}}} \log\left|\frac{\frac{1}{\sqrt{2}} + v}{\frac{1}{\sqrt{2}} - v}\right|\right] = \log|x| + \log C \)
\( \frac{1}{2} \left[\frac{\sqrt{2}}{2} \log\left|\frac{1 + \sqrt{2}v}{1 - \sqrt{2}v}\right|\right] = \log|x| + \log C \)
\( \frac{\sqrt{2}}{4} \log\left|\frac{1 + \sqrt{2}v}{1 - \sqrt{2}v}\right| = \log|x| + \log C \)
Substitute back \( v = \frac{y}{x} \):
\( \frac{\sqrt{2}}{4} \log\left|\frac{1 + \sqrt{2}\frac{y}{x}}{1 - \sqrt{2}\frac{y}{x}}\right| = \log|x| + \log C \)
\( \frac{\sqrt{2}}{4} \log\left|\frac{x + \sqrt{2}y}{x - \sqrt{2}y}\right| = \log|x| + \log C \)
This is the general solution.

In simple words: First, we put the equation in \( \frac{dy}{dx} \) form and verified it was homogeneous. Next, we used the substitution \( y = vx \) to make the equation separable. We then split the \( v \) and \( x \) terms and integrated them. Finally, we substituted \( \frac{y}{x} \) back for \( v \) to complete the solution.

Exam Tip: Be mindful of using the correct integral formulas, especially for inverse trigonometric or logarithmic forms. Also, keep track of constants and simplify the final answer by substituting back \( v = \frac{y}{x} \).

 

Question 6. \( x dy - y dx = \sqrt{x^2+y^2} dx \)
Answer: We have the given differential equation \( x dy - y dx = \sqrt{x^2+y^2} dx \).
Rearrange the terms to get \( \frac{dy}{dx} \):
\( x dy = y dx + \sqrt{x^2+y^2} dx \)
\( x dy = (y + \sqrt{x^2+y^2}) dx \)
\( \frac{dy}{dx} = \frac{y + \sqrt{x^2+y^2}}{x} = f(x, y) \)
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{\lambda y + \sqrt{(\lambda x)^2+(\lambda y)^2}}{\lambda x} \)
\( = \frac{\lambda y + \sqrt{\lambda^2 x^2+\lambda^2 y^2}}{\lambda x} \)
\( = \frac{\lambda y + \lambda \sqrt{x^2+y^2}}{\lambda x} \)
\( = \frac{\lambda (y + \sqrt{x^2+y^2})}{\lambda x} \)
\( = \lambda^0 \left(\frac{y + \sqrt{x^2+y^2}}{x}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into the equation:
\( v + x \frac{dv}{dx} = \frac{vx + \sqrt{x^2+(vx)^2}}{x} \)
\( v + x \frac{dv}{dx} = \frac{vx + \sqrt{x^2+v^2 x^2}}{x} \)
\( v + x \frac{dv}{dx} = \frac{vx + \sqrt{x^2(1+v^2)}}{x} \)
\( v + x \frac{dv}{dx} = \frac{vx + |x|\sqrt{1+v^2}}{x} \)
Assuming \( x > 0 \), then \( |x| = x \):
\( v + x \frac{dv}{dx} = \frac{vx + x\sqrt{1+v^2}}{x} \)
\( v + x \frac{dv}{dx} = v + \sqrt{1+v^2} \)
Now, separate the variables:
\( x \frac{dv}{dx} = \sqrt{1+v^2} \)
\( \frac{dv}{\sqrt{1+v^2}} = \frac{dx}{x} \)
Now, integrate both sides:
\( \int \frac{dv}{\sqrt{1+v^2}} = \int \frac{1}{x} dx \)
Using the standard integral formula \( \int \frac{1}{\sqrt{a^2+x^2}} dx = \log|x + \sqrt{a^2+x^2}| \), where \( a=1 \):
\( \log|v + \sqrt{1+v^2}| = \log|x| + \log C \)
\( \log|v + \sqrt{1+v^2}| = \log|Cx| \)
\( v + \sqrt{1+v^2} = Cx \)
Substitute back \( v = \frac{y}{x} \):
\( \frac{y}{x} + \sqrt{1+\left(\frac{y}{x}\right)^2} = Cx \)
\( \frac{y}{x} + \sqrt{1+\frac{y^2}{x^2}} = Cx \)
\( \frac{y}{x} + \sqrt{\frac{x^2+y^2}{x^2}} = Cx \)
\( \frac{y}{x} + \frac{\sqrt{x^2+y^2}}{|x|} = Cx \)
Assuming \( x > 0 \), then \( |x| = x \):
\( \frac{y + \sqrt{x^2+y^2}}{x} = Cx \)
\( y + \sqrt{x^2+y^2} = Cx^2 \)
This is the general solution.

In simple words: We first put the equation into the \( \frac{dy}{dx} \) format and verified its homogeneous nature. Then, we used the substitution \( y = vx \) to simplify the equation. After separating the \( v \) and \( x \) terms, we integrated both sides. Finally, we substituted \( \frac{y}{x} \) back for \( v \) to get the final solution.

Exam Tip: When dealing with square roots like \( \sqrt{x^2+y^2} \), remember that \( \sqrt{x^2(1+v^2)} = |x|\sqrt{1+v^2} \). Often, it's assumed \( x>0 \) in these problems, allowing you to replace \( |x| \) with \( x \). Be sure to use the correct integration formula for \( \int \frac{dv}{\sqrt{1+v^2}} \).

 

Question 7. \( \left\{x \cos\left(\frac{y}{x}\right) + y \sin\left(\frac{y}{x}\right)\right\} y dx = \left\{y \sin\left(\frac{y}{x}\right) - x \cos\left(\frac{y}{x}\right)\right\} x dy \)
Answer: We have the given differential equation:
\( \left\{x \cos\left(\frac{y}{x}\right) + y \sin\left(\frac{y}{x}\right)\right\} y dx = \left\{y \sin\left(\frac{y}{x}\right) - x \cos\left(\frac{y}{x}\right)\right\} x dy \)
Rearrange to express in the form \( \frac{dy}{dx} \):
\( \frac{dy}{dx} = \frac{\left\{x \cos\left(\frac{y}{x}\right) + y \sin\left(\frac{y}{x}\right)\right\} y}{\left\{y \sin\left(\frac{y}{x}\right) - x \cos\left(\frac{y}{x}\right)\right\} x} = f(x, y) \)
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{\left\{\lambda x \cos\left(\frac{\lambda y}{\lambda x}\right) + \lambda y \sin\left(\frac{\lambda y}{\lambda x}\right)\right\} \lambda y}{\left\{\lambda y \sin\left(\frac{\lambda y}{\lambda x}\right) - \lambda x \cos\left(\frac{\lambda y}{\lambda x}\right)\right\} \lambda x} \)
\( = \frac{\lambda^2 \left\{x \cos\left(\frac{y}{x}\right) + y \sin\left(\frac{y}{x}\right)\right\} y}{\lambda^2 \left\{y \sin\left(\frac{y}{x}\right) - x \cos\left(\frac{y}{x}\right)\right\} x} \)
\( = \lambda^0 \left(\frac{\left\{x \cos\left(\frac{y}{x}\right) + y \sin\left(\frac{y}{x}\right)\right\} y}{\left\{y \sin\left(\frac{y}{x}\right) - x \cos\left(\frac{y}{x}\right)\right\} x}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into the equation:
\( v + x \frac{dv}{dx} = \frac{\left\{x \cos\left(\frac{vx}{x}\right) + vx \sin\left(\frac{vx}{x}\right)\right\} vx}{\left\{vx \sin\left(\frac{vx}{x}\right) - x \cos\left(\frac{vx}{x}\right)\right\} x} \)
\( v + x \frac{dv}{dx} = \frac{\left\{x \cos v + vx \sin v\right\} vx}{\left\{vx \sin v - x \cos v\right\} x} \)
\( v + x \frac{dv}{dx} = \frac{x v(\cos v + v \sin v)}{x^2 (v \sin v - \cos v)} \)
\( v + x \frac{dv}{dx} = \frac{v(\cos v + v \sin v)}{v \sin v - \cos v} \)
Now, separate the variables:
\( x \frac{dv}{dx} = \frac{v(\cos v + v \sin v)}{v \sin v - \cos v} - v \)
\( x \frac{dv}{dx} = \frac{v \cos v + v^2 \sin v - v(v \sin v - \cos v)}{v \sin v - \cos v} \)
\( x \frac{dv}{dx} = \frac{v \cos v + v^2 \sin v - v^2 \sin v + v \cos v}{v \sin v - \cos v} \)
\( x \frac{dv}{dx} = \frac{2v \cos v}{v \sin v - \cos v} \)
\( \frac{v \sin v - \cos v}{2v \cos v} dv = \frac{dx}{x} \)
\( \left(\frac{v \sin v}{2v \cos v} - \frac{\cos v}{2v \cos v}\right) dv = \frac{dx}{x} \)
\( \left(\frac{1}{2} \tan v - \frac{1}{2v}\right) dv = \frac{dx}{x} \)
Now, integrate both sides:
\( \int \left(\frac{1}{2} \tan v - \frac{1}{2v}\right) dv = \int \frac{1}{x} dx \)
\( \frac{1}{2} \int \tan v dv - \frac{1}{2} \int \frac{1}{v} dv = \int \frac{1}{x} dx \)
\( \frac{1}{2} \log|\sec v| - \frac{1}{2} \log|v| = \log|x| + \log C \)
\( \frac{1}{2} (\log|\sec v| - \log|v|) = \log|x| + \log C \)
\( \frac{1}{2} \log\left|\frac{\sec v}{v}\right| = \log|Cx| \)
\( \log\left|\frac{\sec v}{v}\right|^{1/2} = \log|Cx| \)
\( \sqrt{\frac{\sec v}{v}} = Cx \)
Substitute back \( v = \frac{y}{x} \):
\( \sqrt{\frac{\sec(\frac{y}{x})}{\frac{y}{x}}} = Cx \)
\( \sqrt{\frac{x \sec(\frac{y}{x})}{y}} = Cx \)
Squaring both sides:
\( \frac{x \sec(\frac{y}{x})}{y} = C^2 x^2 \)
\( \sec\left(\frac{y}{x}\right) = C^2 xy \)
\( \frac{1}{\cos(\frac{y}{x})} = C^2 xy \)
\( 1 = C^2 xy \cos\left(\frac{y}{x}\right) \)
Let \( K = C^2 \).
\( K xy \cos\left(\frac{y}{x}\right) = 1 \)
This is the general solution.

In simple words: This was a complex homogeneous equation. We first wrote it in \( \frac{dy}{dx} \) form and proved its homogeneity. Using \( y = vx \) to replace \( y \) and \( \frac{dy}{dx} \), we simplified the equation. After separating the \( v \) and \( x \) terms, we integrated them, using known formulas for tan and log. Finally, we substituted \( \frac{y}{x} \) back for \( v \) and simplified the answer.

Exam Tip: For complex trigonometric homogeneous equations, the algebra after substitution can be lengthy. Carefully simplify terms, use trigonometric identities like \( \sec v = \frac{1}{\cos v} \), and remember to include the constant of integration. Double-check the integration of \( \tan v \) and \( \frac{1}{v} \).

 

Question 8. \( x \frac{dy}{dx} - y + x \sin \frac{y}{x} = 0 \)
Answer: We have the given differential equation \( x \frac{dy}{dx} - y + x \sin \frac{y}{x} = 0 \).
Rearrange to express in the form \( \frac{dy}{dx} \):
\( x \frac{dy}{dx} = y - x \sin \frac{y}{x} \)
\( \frac{dy}{dx} = \frac{y - x \sin \frac{y}{x}}{x} \)
\( \frac{dy}{dx} = \frac{y}{x} - \sin \frac{y}{x} = f(x, y) \)
To show that \( f(x, y) \) is a homogeneous function, we replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{\lambda y}{\lambda x} - \sin \left(\frac{\lambda y}{\lambda x}\right) \)
\( = \frac{y}{x} - \sin \left(\frac{y}{x}\right) \)
\( = \lambda^0 \left(\frac{y}{x} - \sin \frac{y}{x}\right) \)
\( = \lambda^0 f(x, y) \)
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve the differential equation, we make the substitution \( y = vx \), which means \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substitute \( y = vx \) and \( \frac{dy}{dx} \) into the equation:
\( v + x \frac{dv}{dx} = \frac{vx}{x} - \sin \left(\frac{vx}{x}\right) \)
\( v + x \frac{dv}{dx} = v - \sin v \)
Now, separate the variables:
\( x \frac{dv}{dx} = v - \sin v - v \)
\( x \frac{dv}{dx} = -\sin v \)
\( \frac{dv}{\sin v} = -\frac{dx}{x} \)
\( \csc v dv = -\frac{dx}{x} \)
Now, integrate both sides:
\( \int \csc v dv = -\int \frac{1}{x} dx \)
\( \log|\csc v - \cot v| = -\log|x| + \log C \)
\( \log|\csc v - \cot v| = \log\left|\frac{C}{x}\right| \)
\( \csc v - \cot v = \frac{C}{x} \)
Substitute back \( v = \frac{y}{x} \):
\( \csc\left(\frac{y}{x}\right) - \cot\left(\frac{y}{x}\right) = \frac{C}{x} \)
We can also write this using sine and cosine:
\( \frac{1}{\sin(\frac{y}{x})} - \frac{\cos(\frac{y}{x})}{\sin(\frac{y}{x})} = \frac{C}{x} \)
\( \frac{1 - \cos(\frac{y}{x})}{\sin(\frac{y}{x})} = \frac{C}{x} \)
\( x \left(1 - \cos\left(\frac{y}{x}\right)\right) = C \sin\left(\frac{y}{x}\right) \)
This is the general solution.

In simple words: First, we rearranged the equation into the \( \frac{dy}{dx} \) form. We then confirmed it was a homogeneous equation. Using the substitution \( y = vx \), we simplified the equation to separate the \( v \) and \( x \) terms. We integrated both sides using standard integral formulas. Finally, we substituted \( \frac{y}{x} \) back for \( v \) and simplified the expression to get the solution.

Exam Tip: Be familiar with the integral of \( \csc v \), which is \( \log|\csc v - \cot v| \). After substitution, it's often helpful to convert the trigonometric terms back to sine and cosine to simplify the expression further.

 

Question 9. \( y dx + x \log \left(\frac{y}{x}\right) dy - 2x dy = 0 \)
Answer: We have the given differential equation \( y dx + x \log \left(\frac{y}{x}\right) dy - 2x dy = 0 \).
Rearrange to express in the form \( \frac{dy}{dx} \):
\( y dx = \left(2x - x \log \left(\frac{y}{x}\right)\right) dy \)
\( \frac{dx}{dy} = \frac{2x - x \log \left(\frac{y}{x}\right)}{y} \)
\( \frac{dx}{dy} = \frac{x \left(2 - \log \left(\frac{y}{x}\right)\right)}{y} \)
This equation is of the form \( \frac{dx}{dy} = g\left(\frac{x}{y}\right) \). So, it's a homogeneous equation. We will use the substitution \( x = vy \) instead of \( y = vx \).
Let \( x = vy \), then \( \frac{dx}{dy} = v + y \frac{dv}{dy} \).
Substitute \( x = vy \) and \( \frac{dx}{dy} \) into the equation:
\( v + y \frac{dv}{dy} = \frac{vy \left(2 - \log \left(\frac{vy}{y}\right)\right)}{y} \)
\( v + y \frac{dv}{dy} = v \left(2 - \log v\right) \)
\( v + y \frac{dv}{dy} = 2v - v \log v \)
Now, separate the variables:
\( y \frac{dv}{dy} = 2v - v \log v - v \)
\( y \frac{dv}{dy} = v - v \log v \)
\( y \frac{dv}{dy} = v(1 - \log v) \)
\( \frac{dv}{v(1 - \log v)} = \frac{dy}{y} \)
Now, integrate both sides:
\( \int \frac{dv}{v(1 - \log v)} = \int \frac{1}{y} dy \)
For the left integral, let \( t = 1 - \log v \). Then \( dt = -\frac{1}{v} dv \), so \( \frac{1}{v} dv = -dt \).
\( \int \frac{-dt}{t} = \int \frac{1}{y} dy \)
\( -\log|t| = \log|y| + \log C \)
\( -\log|1 - \log v| = \log|Cy| \)
\( \log|1 - \log v|^{-1} = \log|Cy| \)
\( \frac{1}{|1 - \log v|} = Cy \)
\( \frac{1}{1 - \log v} = \pm Cy \)
Let \( \pm C = K \), a new constant.
\( 1 - \log v = \frac{1}{Ky} \)
\( \log v = 1 - \frac{1}{Ky} \)
Substitute back \( v = \frac{x}{y} \):
\( \log\left(\frac{x}{y}\right) = 1 - \frac{1}{Ky} \)
This is the general solution.

In simple words: This equation was homogeneous, but in terms of \( \frac{dx}{dy} \) and \( \frac{x}{y} \). So, we used the substitution \( x = vy \) and its derivative. After simplifying and separating the \( v \) and \( y \) terms, we integrated both sides. A substitution was needed for the \( v \) integral. Finally, we replaced \( v \) with \( \frac{x}{y} \) to get the solution.

Exam Tip: Be careful to identify whether the differential equation is homogeneous in terms of \( \frac{dy}{dx} \) or \( \frac{dx}{dy} \). This determines whether to use \( y=vx \) or \( x=vy \) substitution. Also, remember the substitution rule for integration, especially for logarithmic terms.

 

Question 10. \( (1 + e^{\frac{x}{y}})dx + e^{\frac{x}{y}}\left(1 - \frac{x}{y}\right)dy = 0 \)
Answer: We have the given differential equation \( (1 + e^{\frac{x}{y}})dx + e^{\frac{x}{y}}\left(1 - \frac{x}{y}\right)dy = 0 \).
Rearrange to express in the form \( \frac{dx}{dy} \):
\( (1 + e^{\frac{x}{y}})dx = -e^{\frac{x}{y}}\left(1 - \frac{x}{y}\right)dy \)
\( \frac{dx}{dy} = \frac{-e^{\frac{x}{y}}\left(1 - \frac{x}{y}\right)}{1 + e^{\frac{x}{y}}} = g\left(\frac{x}{y}\right) \)
This equation is of the form \( \frac{dx}{dy} = g\left(\frac{x}{y}\right) \). So, it's a homogeneous equation. We will use the substitution \( x = vy \) instead of \( y = vx \).
Let \( x = vy \), then \( \frac{dx}{dy} = v + y \frac{dv}{dy} \).
Substitute \( x = vy \) and \( \frac{dx}{dy} \) into the equation:
\( v + y \frac{dv}{dy} = \frac{-e^{\frac{vy}{y}}\left(1 - \frac{vy}{y}\right)}{1 + e^{\frac{vy}{y}}} \)
\( v + y \frac{dv}{dy} = \frac{-e^v(1 - v)}{1 + e^v} \)
Now, separate the variables:
\( y \frac{dv}{dy} = \frac{-e^v(1 - v)}{1 + e^v} - v \)
\( y \frac{dv}{dy} = \frac{-e^v + ve^v - v(1 + e^v)}{1 + e^v} \)
\( y \frac{dv}{dy} = \frac{-e^v + ve^v - v - ve^v}{1 + e^v} \)
\( y \frac{dv}{dy} = \frac{-e^v - v}{1 + e^v} \)
\( y \frac{dv}{dy} = -\frac{v + e^v}{1 + e^v} \)
\( \frac{1 + e^v}{v + e^v} dv = -\frac{dy}{y} \)
Now, integrate both sides:
\( \int \frac{1 + e^v}{v + e^v} dv = -\int \frac{1}{y} dy \)
For the left integral, let \( t = v + e^v \). Then \( dt = (1 + e^v) dv \).
\( \int \frac{dt}{t} = -\int \frac{1}{y} dy \)
\( \log|t| = -\log|y| + \log C \)
\( \log|v + e^v| = \log\left|\frac{C}{y}\right| \)
\( v + e^v = \frac{C}{y} \)
Substitute back \( v = \frac{x}{y} \):
\( \frac{x}{y} + e^{\frac{x}{y}} = \frac{C}{y} \)
Multiply the entire equation by \( y \):
\( x + y e^{\frac{x}{y}} = C \)
This is the general solution.

In simple words: This equation was given in a form that suggested using \( \frac{dx}{dy} \) and \( \frac{x}{y} \). We confirmed its homogeneous nature. We then used the substitution \( x = vy \) to simplify the equation. After separating the \( v \) and \( y \) terms, we integrated both sides. A substitution was helpful for the \( v \) integral. Finally, we replaced \( v \) with \( \frac{x}{y} \) to get the final solution.

Exam Tip: For equations involving \( e^{\frac{x}{y}} \) or \( e^{\frac{y}{x}} \), the appropriate substitution is usually \( x=vy \) or \( y=vx \) respectively. Recognizing the integral of the form \( \int \frac{f'(x)}{f(x)} dx \) is crucial for efficiency in solving these types of problems.

 

Question 11. (x + y)dy + (x - y)dx = 0, y = 1, when x = 1.
Answer: We are given the differential equation \( (x + y)dy + (x - y)dx = 0 \).
We can rearrange this equation to find \( \frac{dy}{dx} \):
\( (x + y)dy = -(x - y)dx \)
\( \implies \frac{dy}{dx} = -\frac{x - y}{x + y} = \frac{y - x}{y + x} \).
Let \( f(x, y) = \frac{y - x}{y + x} \).
Replacing \( x \) by \( \lambda x \) and \( y \) by \( \lambda y \), we get:
\( f(\lambda x, \lambda y) = \frac{\lambda y - \lambda x}{\lambda y + \lambda x} = \frac{\lambda (y - x)}{\lambda (y + x)} = \frac{y - x}{y + x} = \lambda^0 f(x, y) \).
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the function \( f(x, y) \) is a homogeneous function of degree zero.
To solve this homogeneous equation, we substitute \( y = vx \), which gives \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substituting these into the differential equation:
\( v + x \frac{dv}{dx} = \frac{vx - x}{vx + x} \)
\( \implies v + x \frac{dv}{dx} = \frac{x(v - 1)}{x(v + 1)} \)
\( \implies v + x \frac{dv}{dx} = \frac{v - 1}{v + 1} \)
\( \implies x \frac{dv}{dx} = \frac{v - 1}{v + 1} - v \)
\( \implies x \frac{dv}{dx} = \frac{v - 1 - v(v + 1)}{v + 1} \)
\( \implies x \frac{dv}{dx} = \frac{v - 1 - v^2 - v}{v + 1} \)
\( \implies x \frac{dv}{dx} = \frac{-1 - v^2}{v + 1} \)
\( \implies x \frac{dv}{dx} = -\frac{v^2 + 1}{v + 1} \).
Now, we separate the variables:
\( \frac{v + 1}{v^2 + 1} dv = -\frac{dx}{x} \).
Integrate both sides:
\( \int \frac{v + 1}{v^2 + 1} dv = -\int \frac{dx}{x} \)
\( \implies \int \frac{v}{v^2 + 1} dv + \int \frac{1}{v^2 + 1} dv = -\int \frac{dx}{x} \).
For the first integral, let \( t = v^2 + 1 \), so \( dt = 2v dv \implies v dv = \frac{1}{2} dt \).
\( \implies \frac{1}{2} \int \frac{dt}{t} + \int \frac{1}{v^2 + 1} dv = -\int \frac{dx}{x} \)
\( \implies \frac{1}{2} \log|t| + \arctan(v) = -\log|x| + C \)
Substitute back \( t = v^2 + 1 \):
\( \implies \frac{1}{2} \log(v^2 + 1) + \arctan(v) = -\log|x| + C \).
Now substitute \( v = \frac{y}{x} \):
\( \implies \frac{1}{2} \log\left(\left(\frac{y}{x}\right)^2 + 1\right) + \arctan\left(\frac{y}{x}\right) = -\log|x| + C \)
\( \implies \frac{1}{2} \log\left(\frac{y^2 + x^2}{x^2}\right) + \arctan\left(\frac{y}{x}\right) = -\log|x| + C \)
\( \implies \frac{1}{2} (\log(y^2 + x^2) - \log(x^2)) + \arctan\left(\frac{y}{x}\right) = -\log|x| + C \)
\( \implies \frac{1}{2} \log(x^2 + y^2) - \log|x| + \arctan\left(\frac{y}{x}\right) = -\log|x| + C \)
\( \implies \frac{1}{2} \log(x^2 + y^2) + \arctan\left(\frac{y}{x}\right) = C \).
We are given the condition \( y = 1 \) when \( x = 1 \). Substitute these values to find \( C \):
\( \frac{1}{2} \log(1^2 + 1^2) + \arctan\left(\frac{1}{1}\right) = C \)
\( \implies \frac{1}{2} \log(2) + \arctan(1) = C \)
\( \implies \frac{1}{2} \log(2) + \frac{\pi}{4} = C \).
Therefore, the particular solution is:
\( \frac{1}{2} \log(x^2 + y^2) + \arctan\left(\frac{y}{x}\right) = \frac{1}{2} \log(2) + \frac{\pi}{4} \).
In simple words: First, we change the given equation into a standard form. Then, we check if it is homogeneous, which means all terms have the same total power. We use a special trick by replacing \( y \) with \( vx \) to simplify the equation, then separate the \( v \) and \( x \) terms. After integrating both sides, we put \( y/x \) back in for \( v \). Finally, we use the given starting values for \( x \) and \( y \) to find the constant \( C \), giving us the exact solution for those specific conditions.

Exam Tip: Remember to always check for homogeneity first, then use the substitution \( y = vx \) for \( dy/dx \) type equations or \( x = vy \) for \( dx/dy \) type equations. Don't forget to evaluate the constant of integration \( C \) using the given initial conditions to find the particular solution.

 

Question 12. x²dy + (xy + y²)dx = 0, y = 1, when x = 1.
Answer: We are given the differential equation \( x^2 dy + (xy + y^2) dx = 0 \).
First, we rearrange it to find \( \frac{dy}{dx} \):
\( x^2 dy = -(xy + y^2) dx \)
\( \implies \frac{dy}{dx} = -\frac{xy + y^2}{x^2} \).
Let \( f(x, y) = -\frac{xy + y^2}{x^2} \).
To check if it is homogeneous, we replace \( x \) by \( \lambda x \) and \( y \) by \( \lambda y \):
\( f(\lambda x, \lambda y) = -\frac{(\lambda x)(\lambda y) + (\lambda y)^2}{(\lambda x)^2} \)
\( \implies f(\lambda x, \lambda y) = -\frac{\lambda^2 xy + \lambda^2 y^2}{\lambda^2 x^2} \)
\( \implies f(\lambda x, \lambda y) = -\frac{\lambda^2 (xy + y^2)}{\lambda^2 x^2} \)
\( \implies f(\lambda x, \lambda y) = -\frac{xy + y^2}{x^2} = \lambda^0 f(x, y) \).
Since \( f(\lambda x, \lambda y) = \lambda^0 f(x, y) \), the differential equation is homogeneous.
Now, we use the substitution \( y = vx \), which implies \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
Substituting these into the equation:
\( v + x \frac{dv}{dx} = -\frac{x(vx) + (vx)^2}{x^2} \)
\( \implies v + x \frac{dv}{dx} = -\frac{vx^2 + v^2 x^2}{x^2} \)
\( \implies v + x \frac{dv}{dx} = -\frac{x^2(v + v^2)}{x^2} \)
\( \implies v + x \frac{dv}{dx} = -(v + v^2) \)
\( \implies x \frac{dv}{dx} = -v - v^2 - v \)
\( \implies x \frac{dv}{dx} = -(2v + v^2) \).
Separating the variables, we get:
\( \frac{dv}{v^2 + 2v} = -\frac{dx}{x} \).
Integrate both sides:
\( \int \frac{dv}{v(v + 2)} = -\int \frac{dx}{x} \).
We use partial fraction decomposition for the left side:
\( \frac{1}{v(v + 2)} = \frac{A}{v} + \frac{B}{v + 2} \)
\( \implies 1 = A(v + 2) + Bv \).
If \( v = 0 \), then \( 1 = 2A \implies A = \frac{1}{2} \).
If \( v = -2 \), then \( 1 = -2B \implies B = -\frac{1}{2} \).
So, \( \int \left(\frac{1/2}{v} - \frac{1/2}{v + 2}\right) dv = -\int \frac{dx}{x} \)
\( \implies \frac{1}{2} \int \left(\frac{1}{v} - \frac{1}{v + 2}\right) dv = -\int \frac{dx}{x} \)
\( \implies \frac{1}{2} (\log|v| - \log|v + 2|) = -\log|x| + C' \)
\( \implies \frac{1}{2} \log\left|\frac{v}{v + 2}\right| = -\log|x| + C' \)
\( \implies \log\left|\frac{v}{v + 2}\right| = -2\log|x| + 2C' \)
\( \implies \log\left|\frac{v}{v + 2}\right| = \log|x^{-2}| + \log|K| \) (where \( \log K = 2C' \))
\( \implies \frac{v}{v + 2} = \frac{K}{x^2} \).
Substitute back \( v = \frac{y}{x} \):
\( \frac{y/x}{y/x + 2} = \frac{K}{x^2} \)
\( \implies \frac{y/x}{(y + 2x)/x} = \frac{K}{x^2} \)
\( \implies \frac{y}{y + 2x} = \frac{K}{x^2} \)
\( \implies x^2 y = K(y + 2x) \).
We are given \( y = 1 \) when \( x = 1 \). Substitute these values to find \( K \):
\( (1)^2 (1) = K(1 + 2(1)) \)
\( \implies 1 = K(3) \)
\( \implies K = \frac{1}{3} \).
So, the particular solution is:
\( x^2 y = \frac{1}{3}(y + 2x) \)
\( \implies 3x^2 y = y + 2x \).
In simple words: We first rewrite the equation to find \( dy/dx \). Then, we check if it's homogeneous by changing \( x \) and \( y \) with \( \lambda x \) and \( \lambda y \). Since it is, we replace \( y \) with \( vx \) and \( dy/dx \) with \( v + x(dv/dx) \). This lets us separate the \( v \) and \( x \) parts, which we can then integrate. After integrating, we change \( v \) back to \( y/x \) and use the given initial values for \( x \) and \( y \) to calculate the constant \( K \), giving us the final specific solution.

Exam Tip: For problems involving integration of rational functions like \( \frac{1}{v^2 + 2v} \), remember to use partial fraction decomposition to simplify the integrand before integrating. This is a common step in solving homogeneous differential equations.

 

Question 13. (x sin² \( \frac{y}{x} \) – y) dx + x dy = 0, y = \( \frac{\pi}{4} \), when x = 1.
Answer: We are given the differential equation \( (x \sin^2 \left(\frac{y}{x}\right) - y) dx + x dy = 0 \).
Rearranging to find \( \frac{dy}{dx} \):
\( x dy = -(x \sin^2 \left(\frac{y}{x}\right) - y) dx \)
\( \implies \frac{dy}{dx} = -\frac{x \sin^2 \left(\frac{y}{x}\right) - y}{x} \)
\( \implies \frac{dy}{dx} = \frac{y - x \sin^2 \left(\frac{y}{x}\right)}{x} \).
Let \( f(x, y) = \frac{y - x \sin^2 \left(\frac{y}{x}\right)}{x} \).
To check for homogeneity, replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{\lambda y - \lambda x \sin^2 \left(\frac{\lambda y}{\lambda x}\right)}{\lambda x} \)
\( \implies f(\lambda x, \lambda y) = \frac{\lambda y - \lambda x \sin^2 \left(\frac{y}{x}\right)}{\lambda x} \)
\( \implies f(\lambda x, \lambda y) = \frac{\lambda \left(y - x \sin^2 \left(\frac{y}{x}\right)\right)}{\lambda x} \)
\( \implies f(\lambda x, \lambda y) = \frac{y - x \sin^2 \left(\frac{y}{x}\right)}{x} = \lambda^0 f(x, y) \).
The equation is homogeneous.
Substitute \( y = vx \), so \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
\( v + x \frac{dv}{dx} = \frac{vx - x \sin^2(v)}{x} \)
\( \implies v + x \frac{dv}{dx} = v - \sin^2(v) \)
\( \implies x \frac{dv}{dx} = -\sin^2(v) \).
Separating variables:
\( \frac{dv}{\sin^2(v)} = -\frac{dx}{x} \)
\( \implies \csc^2(v) dv = -\frac{dx}{x} \).
Integrate both sides:
\( \int \csc^2(v) dv = -\int \frac{dx}{x} \)
\( \implies -\cot(v) = -\log|x| + C \)
\( \implies \cot(v) = \log|x| - C \).
Substitute back \( v = \frac{y}{x} \):
\( \cot\left(\frac{y}{x}\right) = \log|x| - C \).
We are given \( y = \frac{\pi}{4} \) when \( x = 1 \). Substitute these values:
\( \cot\left(\frac{\pi/4}{1}\right) = \log|1| - C \)
\( \implies \cot\left(\frac{\pi}{4}\right) = 0 - C \)
\( \implies 1 = -C \implies C = -1 \).
So, the particular solution is:
\( \cot\left(\frac{y}{x}\right) = \log|x| - (-1) \)
\( \implies \cot\left(\frac{y}{x}\right) = \log|x| + 1 \).
In simple words: We begin by changing the equation into the \( dy/dx \) form. We then check if it's homogeneous, which means it stays the same when we multiply \( x \) and \( y \) by a constant. Because it is, we replace \( y \) with \( vx \) and \( dy/dx \) with \( v + x(dv/dx) \) to make it simpler. After this, we separate the \( v \) and \( x \) terms and integrate them. Finally, we put \( y/x \) back for \( v \) and use the given starting values for \( x \) and \( y \) to find the constant, giving us the exact answer for those specific conditions.

Exam Tip: When integrating trigonometric functions, ensure you remember standard integrals like \( \int \csc^2(v) dv = -\cot(v) \). Also, accurately handling the constant of integration and applying initial conditions are crucial for finding the correct particular solution.

 

Question 14. \( \frac{dy}{dx} – \frac{y}{x} + \csc \left(\frac{y}{x}\right) = 0 \), y = 0, when x = 1.
Answer: We are given the differential equation \( \frac{dy}{dx} – \frac{y}{x} + \csc \left(\frac{y}{x}\right) = 0 \).
Rearranging it:
\( \frac{dy}{dx} = \frac{y}{x} - \csc \left(\frac{y}{x}\right) \).
Let \( f(x, y) = \frac{y}{x} - \csc \left(\frac{y}{x}\right) \).
To check for homogeneity, replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{\lambda y}{\lambda x} - \csc \left(\frac{\lambda y}{\lambda x}\right) \)
\( \implies f(\lambda x, \lambda y) = \frac{y}{x} - \csc \left(\frac{y}{x}\right) = \lambda^0 f(x, y) \).
The equation is homogeneous.
Substitute \( y = vx \), so \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
\( v + x \frac{dv}{dx} = v - \csc(v) \)
\( \implies x \frac{dv}{dx} = -\csc(v) \).
Separating variables:
\( \frac{dv}{\csc(v)} = -\frac{dx}{x} \)
\( \implies \sin(v) dv = -\frac{dx}{x} \).
Integrate both sides:
\( \int \sin(v) dv = -\int \frac{dx}{x} \)
\( \implies -\cos(v) = -\log|x| + C' \)
\( \implies \cos(v) = \log|x| - C' \). Let \( C = -C' \).
\( \implies \cos(v) = \log|x| + C \).
Substitute back \( v = \frac{y}{x} \):
\( \cos\left(\frac{y}{x}\right) = \log|x| + C \).
We are given \( y = 0 \) when \( x = 1 \). Substitute these values:
\( \cos\left(\frac{0}{1}\right) = \log|1| + C \)
\( \implies \cos(0) = 0 + C \)
\( \implies 1 = C \).
So, the particular solution is:
\( \cos\left(\frac{y}{x}\right) = \log|x| + 1 \).
This can also be written as \( \log|x| = \cos\left(\frac{y}{x}\right) - 1 \).
In simple words: We first rewrite the equation to clearly see its form. Since it's homogeneous, meaning all terms have the same overall power, we can use the substitution \( y = vx \). This changes the equation into one where we can easily separate the variables \( v \) and \( x \). After integrating both parts, we replace \( v \) with \( y/x \). Finally, we use the given starting conditions for \( x \) and \( y \) to find the constant value \( C \), which gives us the specific solution for this problem.

Exam Tip: Be careful with signs when integrating and rearranging terms. A common mistake is misplacing a negative sign, which can lead to an incorrect solution. Double-check your algebraic manipulations and integration results.

 

Question 15. 2 xy + y² - 2x² \( \frac{dy}{dx} \) = 0, y = 2, when x = 1.
Answer: We are given the differential equation \( 2xy + y^2 - 2x^2 \frac{dy}{dx} = 0 \).
Rearranging to find \( \frac{dy}{dx} \):
\( 2x^2 \frac{dy}{dx} = 2xy + y^2 \)
\( \implies \frac{dy}{dx} = \frac{2xy + y^2}{2x^2} \).
Let \( f(x, y) = \frac{2xy + y^2}{2x^2} \).
To check for homogeneity, replace \( x \) with \( \lambda x \) and \( y \) with \( \lambda y \):
\( f(\lambda x, \lambda y) = \frac{2(\lambda x)(\lambda y) + (\lambda y)^2}{2(\lambda x)^2} \)
\( \implies f(\lambda x, \lambda y) = \frac{2\lambda^2 xy + \lambda^2 y^2}{2\lambda^2 x^2} \)
\( \implies f(\lambda x, \lambda y) = \frac{\lambda^2 (2xy + y^2)}{\lambda^2 (2x^2)} \)
\( \implies f(\lambda x, \lambda y) = \frac{2xy + y^2}{2x^2} = \lambda^0 f(x, y) \).
The equation is homogeneous.
Substitute \( y = vx \), so \( \frac{dy}{dx} = v + x \frac{dv}{dx} \).
\( v + x \frac{dv}{dx} = \frac{2x(vx) + (vx)^2}{2x^2} \)
\( \implies v + x \frac{dv}{dx} = \frac{2vx^2 + v^2 x^2}{2x^2} \)
\( \implies v + x \frac{dv}{dx} = \frac{x^2(2v + v^2)}{2x^2} \)
\( \implies v + x \frac{dv}{dx} = \frac{2v + v^2}{2} \)
\( \implies x \frac{dv}{dx} = \frac{2v + v^2}{2} - v \)
\( \implies x \frac{dv}{dx} = \frac{2v + v^2 - 2v}{2} \)
\( \implies x \frac{dv}{dx} = \frac{v^2}{2} \).
Separating variables:
\( \frac{2 dv}{v^2} = \frac{dx}{x} \)
\( \implies 2 v^{-2} dv = \frac{dx}{x} \).
Integrate both sides:
\( \int 2 v^{-2} dv = \int \frac{dx}{x} \)
\( \implies 2 \frac{v^{-1}}{-1} = \log|x| + C \)
\( \implies -\frac{2}{v} = \log|x| + C \).
Substitute back \( v = \frac{y}{x} \):
\( -\frac{2}{y/x} = \log|x| + C \)
\( \implies -\frac{2x}{y} = \log|x| + C \).
We are given \( y = 2 \) when \( x = 1 \). Substitute these values:
\( -\frac{2(1)}{2} = \log|1| + C \)
\( \implies -1 = 0 + C \)
\( \implies C = -1 \).
So, the particular solution is:
\( -\frac{2x}{y} = \log|x| - 1 \)
\( \implies 1 - \log|x| = \frac{2x}{y} \)
\( \implies y = \frac{2x}{1 - \log|x|} \).
In simple words: We first rewrite the equation to find \( dy/dx \). After checking that it is homogeneous, we use the substitution \( y = vx \). This allows us to separate the variables \( v \) and \( x \), making the equation easier to integrate. Once integrated, we substitute \( v = y/x \) back into the solution. Finally, we use the given starting values for \( x \) and \( y \) to determine the constant of integration, giving us the specific solution for the problem.

Exam Tip: Pay close attention to the algebraic manipulation when separating variables. Incorrectly grouping terms or signs can lead to errors in integration and, ultimately, the final solution. Remember that \( \int v^{-2} dv = -v^{-1} \).

 

Question 16. A homogeneous differential equation of the form \( \frac{dx}{dy} = h\left(\frac{x}{y}\right) \) can be solved by making the substitution.
(a) y = vx
(b) v = yx
(c) x = vy
(d) x = v
Answer: (c) x = vy
In simple words: When a homogeneous differential equation looks like \( dx/dy = h(x/y) \), it means the right side only depends on the ratio \( x/y \). In this situation, the correct way to simplify and solve it is by replacing \( x \) with \( vy \).

Exam Tip: Remember the rule: if the equation is in the form \( \frac{dy}{dx} = f\left(\frac{y}{x}\right) \), substitute \( y = vx \). If it's in the form \( \frac{dx}{dy} = f\left(\frac{x}{y}\right) \), substitute \( x = vy \). This is a fundamental concept for solving homogeneous differential equations.

 

Question 17. Which of the following is a homogeneous differential equation?
(a) (4x + 6y + 5)dy – (3y + 2x + 4) dx = 0
(b) xy dx – (x³ + y³)dy = 0
(c) (x³ + 2y²) dx + 2xy dy = 0
(d) y²dx + (x² – xy – y²) dy = 0
Answer: (d) y²dx + (x² – xy – y²) dy = 0
In simple words: A homogeneous differential equation is one where all terms have the same total power. For option (D), if you look at each part, like \( y^2 \) or \( x^2 \), they all have a power of 2. This makes the equation balanced and homogeneous. The other options have terms with different total powers, so they are not homogeneous.

Exam Tip: To identify a homogeneous differential equation, check the sum of powers of \( x \) and \( y \) in each term. If the sum is the same for all terms, the equation is homogeneous. Constant terms (like 5 or 4 in option A) automatically make an equation non-homogeneous.

Free study material for Mathematics

GSEB Solutions Class 12 Mathematics Chapter 09 Differential Equations

Students can now access the GSEB Solutions for Chapter 09 Differential Equations prepared by teachers on our website. These solutions cover all questions in exercise in your Class 12 Mathematics textbook. Each answer is updated based on the current academic session as per the latest GSEB syllabus.

Detailed Explanations for Chapter 09 Differential Equations

Our expert teachers have provided step-by-step explanations for all the difficult questions in the Class 12 Mathematics chapter. Along with the final answers, we have also explained the concept behind it to help you build stronger understanding of each topic. This will be really helpful for Class 12 students who want to understand both theoretical and practical questions. By studying these GSEB Questions and Answers your basic concepts will improve a lot.

Benefits of using Mathematics Class 12 Solved Papers

Using our Mathematics solutions regularly students will be able to improve their logical thinking and problem-solving speed. These Class 12 solutions are a guide for self-study and homework assistance. Along with the chapter-wise solutions, you should also refer to our Revision Notes and Sample Papers for Chapter 09 Differential Equations to get a complete preparation experience.

FAQs

Where can I find the latest GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5 for the 2026-27 session?

The complete and updated GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5 is available for free on StudiesToday.com. These solutions for Class 12 Mathematics are as per latest GSEB curriculum.

Are the Mathematics GSEB solutions for Class 12 updated for the new 50% competency-based exam pattern?

Yes, our experts have revised the GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5 as per 2026 exam pattern. All textbook exercises have been solved and have added explanation about how the Mathematics concepts are applied in case-study and assertion-reasoning questions.

How do these Class 12 GSEB solutions help in scoring 90% plus marks?

Toppers recommend using GSEB language because GSEB marking schemes are strictly based on textbook definitions. Our GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5 will help students to get full marks in the theory paper.

Do you offer GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5 in multiple languages like Hindi and English?

Yes, we provide bilingual support for Class 12 Mathematics. You can access GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5 in both English and Hindi medium.

Is it possible to download the Mathematics GSEB solutions for Class 12 as a PDF?

Yes, you can download the entire GSEB Class 12 Maths Solutions Chapter 9 Differential Equations Exercise 9.5 in printable PDF format for offline study on any device.