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Solving an Integral Equation by Differentiating with the FTC

When the unknown function sits both outside and inside an integral with a variable upper limit, differentiate both sides: the FTC turns the integral into a value of the integrand, collapsing the equation into a solvable ODE.

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An integral equation defines an unknown function FF implicitly through an integral whose upper limit is the variable xx, for example

G(F(x))=∫axK(t,F(t)) dt.G\bigl(F(x)\bigr)=\int_{a}^{x} K\bigl(t,F(t)\bigr)\,dt.

The right-hand side is an accumulation function, so the Fundamental Theorem of Calculus applies: differentiating it in xx simply evaluates the integrand at the top limit. That single move removes the integral and leaves an ordinary equation (usually a first-order ODE) for FF.

The algorithm

  1. Differentiate both sides in xx. By the FTC, ddx∫axg(t) dt=g(x)\dfrac{d}{dx}\displaystyle\int_{a}^{x} g(t)\,dt = g(x), so the integral becomes K(x,F(x))K\bigl(x,F(x)\bigr). Differentiate the left side with the chain rule (e.g. ddxF2=2F F′\tfrac{d}{dx}F^{2}=2F\,F').
  2. Simplify to an ODE. Cancel common factors of F(x)F(x) — but only after noting why you may (see step 4). You are usually left with F′(x)=h(x)F'(x)=h(x) or a separable equation.
  3. Get the initial value. Plug x=ax=a into the original equation. The integral from aa to aa is 00, which pins down F(a)F(a).
  4. Solve and integrate. Solve the ODE, fixing the constant with the initial value: F(x)=F(a)+∫axh(t) dtF(x)=F(a)+\int_{a}^{x}h(t)\,dt. Evaluate at the requested point.

Cancelling a factor like F(x)F(x) is only legal where it is nonzero. A hypothesis such as "FF is non-constant" (hence not identically 00) is exactly what licenses the division — never drop that justification.

Mini-example

Suppose FF is non-constant with

F2(x)=∫0xF(t) et dt,x≥0.F^{2}(x)=\int_{0}^{x}F(t)\,e^{\sqrt{t}}\,dt,\qquad x\ge 0.

Differentiate. The FTC gives the right side derivative F(x) exF(x)\,e^{\sqrt{x}}; the chain rule gives 2F(x)F′(x)2F(x)F'(x) on the left:

2F(x)F′(x)=F(x) ex.2F(x)F'(x)=F(x)\,e^{\sqrt{x}}.

Cancel F(x)F(x) (allowed since F≢0F\not\equiv 0):   F′(x)=12ex.\;F'(x)=\tfrac{1}{2}e^{\sqrt{x}}.

Initial value. At x=0x=0 the original equation reads F2(0)=∫00=0F^{2}(0)=\int_{0}^{0}=0, so F(0)=0F(0)=0.

Integrate. With u=tu=\sqrt{t} one finds ∫0x12et dt=(t−1)et∣0x=(x−1)ex+1\int_{0}^{x}\tfrac{1}{2}e^{\sqrt{t}}\,dt=\bigl(\sqrt{t}-1\bigr)e^{\sqrt{t}}\big|_{0}^{x}=(\sqrt{x}-1)e^{\sqrt{x}}+1, so

F(x)=(x−1) ex+1.F(x)=(\sqrt{x}-1)\,e^{\sqrt{x}}+1.

Hence F(4)=(2−1)e2+1=e2+1F(4)=(2-1)e^{2}+1=e^{2}+1.

Exam trick: the instant you see the unknown function under an integral sign with a variable upper limit, differentiate the whole equation — the FTC is doing all the work. And always read off the initial condition by setting xx equal to the lower limit, where the integral vanishes.

فرمول‌های کلیدی

Fundamental Theorem of Calculus (differentiation form)
ddx∫axg(t) dt=g(x)\frac{d}{dx}\int_{a}^{x} g(t)\,dt = g(x)

Differentiating an accumulation function returns the integrand evaluated at the variable upper limit; this is what eliminates the integral.

Leibniz rule (variable upper limit)
ddx∫au(x)g(t) dt=g(u(x)) u′(x)\frac{d}{dx}\int_{a}^{u(x)} g(t)\,dt = g\bigl(u(x)\bigr)\,u'(x)

General form when the upper limit is itself a function of x; the FTC case is u(x)=x.

Recover F by integrating the ODE
F(x)=F(a)+∫axF′(t) dtF(x)=F(a)+\int_{a}^{x} F'(t)\,dt

After solving for F', integrate from the lower limit a, using the initial value F(a) read off the original equation.

#integral-equation#fundamental-theorem-of-calculus#differentiation#ode#initial-value#calculus

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