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Q.The integrating factor of the differential equation 2xdydx−y=32x \frac{dy}{dx} - y = 3 is (A) x\sqrt{x} (B) 1x\frac{1}{\sqrt{x}} (C) exe^x (D) e−xe^{-x}

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To find the integrating factor, we first convert the given differential equation into the standard linear form dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x). From this, we identify P(x)=−12xP(x) = -\frac{1}{2x}, and the integrating factor is calculated as e∫P(x)dxe^{\int P(x) dx}, which evaluates to 1x\frac{1}{\sqrt{x}}.

The integrating factor method is a powerful technique used to solve first-order linear differential equations. A first-order linear differential equation has the general form:

dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x)

where P(x)P(x) and Q(x)Q(x) are functions of xx (or constants).

Why the Integrating Factor?

The core idea is to transform the left-hand side (LHS) of this equation into the derivative of a product. Specifically, we want to make the LHS look like ddx(y⋅some function)\frac{d}{dx} (y \cdot \text{some function}).

Let's say we multiply the entire equation by a function, μ(x)\mu(x), which we call the integrating factor:

μ(x)dydx+μ(x)P(x)y=μ(x)Q(x)\mu(x) \frac{dy}{dx} + \mu(x) P(x)y = \mu(x) Q(x)

Now, consider the product rule for differentiation: ddx(μ(x)y)=μ(x)dydx+ydμdx\frac{d}{dx} (\mu(x) y) = \mu(x) \frac{dy}{dx} + y \frac{d\mu}{dx}.

For our modified LHS to be exactly ddx(μ(x)y)\frac{d}{dx} (\mu(x) y), we need the term μ(x)P(x)y\mu(x) P(x)y to be equal to ydμdxy \frac{d\mu}{dx}.

This means:

μ(x)P(x)=dμdx\mu(x) P(x) = \frac{d\mu}{dx}

This is a separable differential equation for μ(x)\mu(x). We can rewrite it as:

dμμ=P(x)dx\frac{d\mu}{\mu} = P(x) dx

Integrating both sides:

∫dμμ=∫P(x)dx\int \frac{d\mu}{\mu} = \int P(x) dx

log⁡∣μ∣=∫P(x)dx\log|\mu| = \int P(x) dx

Exponentiating both sides (and typically taking the positive value for μ(x)\mu(x) as a convention, and omitting the constant of integration since any constant factor in μ(x)\mu(x) would cancel out later):

μ(x)=e∫P(x)dx\mu(x) = e^{\int P(x) dx}

This μ(x)\mu(x) is the integrating factor. Once we multiply the original equation by this μ(x)\mu(x), the LHS becomes ddx(μ(x)y)\frac{d}{dx} (\mu(x) y), which can then be easily integrated to solve for yy.

Let's apply this method to the given problem.

  1. Convert to Standard Form The given differential equation is 2xdydx−y=32x \frac{dy}{dx} - y = 3. The standard form for a first-order linear differential equation is dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x). To achieve this, we need the coefficient of dydx\frac{dy}{dx} to be 1. We can do this by dividing the entire equation by 2x2x:

2xdydx2x−y2x=32x\frac{2x \frac{dy}{dx}}{2x} - \frac{y}{2x} = \frac{3}{2x}

dydx−12xy=32x\frac{dy}{dx} - \frac{1}{2x} y = \frac{3}{2x}

  1. Identify P(x)P(x) Now, comparing our equation dydx−12xy=32x\frac{dy}{dx} - \frac{1}{2x} y = \frac{3}{2x} with the standard form dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x), we can identify P(x)P(x) and Q(x)Q(x):

P(x)=−12xP(x) = -\frac{1}{2x}

$$ Q(x) = \frac{3}{2x} $$ …

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