GUJCET /Mathematics

Differential equations

Calculus · free study notes · Updated

Differential Equations – GUJCET Mathematics Study Notes

Target: Quick, clear, and exam‑friendly notes for the GUJCET Mathematics syllabus.

Scope: First‑order linear & separable equations, exact equations, second‑order linear equations with constant coefficients, and a touch of the variation‑of‑parameters method.

Format:

  1. Simple explanation
  2. Key points (bullet & table)
  3. Worked example (step‑by‑step)
  4. Quick revision summary

1. Simple Explanation

A differential equation connects an unknown function (y(x)) with its derivatives. It tells how the function changes, not what the function is.

Why it matters:

  • Models real‑world phenomena (population growth, cooling, oscillations, circuits).
  • Provides a systematic way to find (y(x)) that satisfies a given relation.

Typical form (for GUJCET):
[ \frac{dy}{dx} = f(x, y) ] or for second order
[ \frac{d^2y}{dx^2} + p(x)\frac{dy}{dx} + q(x)y = r(x) ]


2. Key Points

Topic What to remember Typical method
1. Separable equations (\displaystyle \frac{dy}{dx}=g(x)h(y)) Separate (y) and (x) → integrate both sides
2. Linear first‑order (\displaystyle \frac{dy}{dx}+P(x)y=Q(x)) Integrating factor (\mu(x)=e^{\int P(x),dx})
3. Exact equations (M(x,y)+N(x,y),dy/dx=0) with (\partial M/\partial y=\partial N/\partial x) Find potential function (\psi(x,y)) s.t. (\psi_x=M,\ \psi_y=N)
4. Bernoulli (\displaystyle \frac{dy}{dx}+P(x)y=Q(x)y^n) Substitute (v=y^{1-n}) → linear in (v)
5. Second‑order linear constant‑coefficient (ay''+by'+cy=r(x)) 1) Solve homogeneous: characteristic (ar^2+br+c=0); 2) Find particular via undetermined coefficients or variation of parameters
6. Variation of parameters For (y''+p(x)y'+q(x)y=r(x)) Use solutions (y_1,y_2) of homogeneous part: (y_p=u_1y_1+u_2y_2) with (u_1',u_2') solving a 2×2 system
7. Initial/Boundary conditions Needed to find the specific solution (unique) Plug into general solution to determine constants

Quick Tips

  • Check separability first – if you can write as (g(x)h(y)), you’re done in a few steps.
  • For linear first‑order, compute (\mu(x)) once and reuse for similar problems.
  • Exactness test: If (\partial M/\partial y \neq \partial N/\partial x), look for an integrating factor depending only on (x) or (y).
  • Characteristic roots: Real distinct → two exponentials; repeated → (e^{rx}) and (xe^{rx}); complex → (e^{\alpha x}(C_1\cos\beta x+C_2\sin\beta x)).

3. Worked Example

Problem (GUJCET style)

Solve the differential equation
[ \frac{dy}{dx} + 2y = x^2, \quad y(0)=1 ]

Step‑by‑Step

  1. Identify type

    • Linear first‑order: (P(x)=2,\ Q(x)=x^2).
  2. Find integrating factor
    [ \mu(x)=e^{\int P(x),dx}=e^{\int 2,dx}=e^{2x} ]

  3. Multiply the equation by (\mu(x))
    [ e^{2x}\frac{dy}{dx} + 2e^{2x}y = x^2e^{2x} ]

    Left side is (\dfrac{d}{dx}!\bigl(e^{2x}y\bigr)).

  4. Integrate both sides
    [ \frac{d}{dx}!\bigl(e^{2x}y\bigr) = x^2e^{2x} ] [ \int \frac{d}{dx}!\bigl(e^{2x}y\bigr),dx = \int x^2e^{2x},dx ] Use integration by parts twice (or a table).
    Result:
    [ e^{2x}y = \frac{e^{2x}}{2}\left(x^2 - x + \frac{1}{2}\right) + C ]

  5. Solve for (y)
    [ y = \frac{1}{2}\left(x^2 - x + \frac{1}{2}\right) + Ce^{-2x} ]

  6. Apply initial condition (y(0)=1)
    [ 1 = \frac{1}{2}\left(0 - 0 + \frac{1}{2}\right) + C \cdot 1 ] [ 1 = \frac{1}{4} + C \quad\Rightarrow\quad C = \frac{3}{4} ]

  7. Final solution

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