Sigma Percentile
JEE Main 2026 (28 January Shift 2)
LEVELJEE Advanced

Animated Solution for Mathematics - Differential Equations: Let be a differentiable function satisfying and let . If and are respectively the points of local minima and local maxima of , then the value of is equal to .........

Enter Numerical Value:

Visualized Solution

Analyze the Integral Equation

  • Given equation:
  • Rewrite to isolate from the integral:

Differentiate using Leibniz Rule

  • Differentiating both sides with respect to .
  • Product Rule on the integral term:
  • Leibniz Rule:

Simplify to a Linear ODE

  • Notice that from the original equation.
  • Substitute this back:
  • Rearrange to standard form:

Finding Integrating Factor

  • Linear ODE form:
  • Here, and
  • Integrating Factor (I.F.) =

Solve the ODE for

  • Multiply by I.F. and integrate:
  • Using Integration by Parts:
  • Result:
  • Simplify:

Apply Initial Condition

  • Find from the original equation:
  • Substitute into the general solution.
  • Final function:

Find the Derivative

  • Given
  • By Leibniz Rule:
  • Substitute :

Identify Critical Points

  • Set to find critical points.
  • Critical points:

Sign Analysis of

  • Check the sign of in each interval.
  • For , all factors are positive, but there is a leading negative sign .
  • At , the power is even (), so the sign does not change .
  • At , the power is odd (), so the sign changes .
  • At , the power is odd (), so the sign changes .

Identify and

  • First Derivative Test:
  • At , changes from to Local Minima. So, .
  • At , changes from to Local Maxima. So, .
  • At , no sign change Point of Inflection.

Final Calculation

  • We need to find the value of .
  • Substitute and .
  • .
  • Final Answer:

The Sigma Insight: Linear Differential Equations

Solution Diagram

Analyzing the Setup

Imagine you are standing before a complex, intimidating integral equation. It feels like a locked door, but every lock has a key. Our journey begins with the equation:
The trap here is the term, which binds and together. By applying the laws of exponents, we rewrite this as .
By pulling the term out of the integral, we transform the equation into:
Now that the variable is isolated, we can apply the Leibniz Rule with confidence.

The Power of the Leibniz Rule

We differentiate both sides with respect to . On the right side, we apply the Product Rule to the term .
The Leibniz Rule states that the derivative of the integral is simply . Applying this, we obtain:
Notice that the term reappears. This is exactly the integral part of our original equation, which we can substitute as .
This substitution simplifies our derivative into a beautiful, linear first-order differential equation:

Solving the ODE

We are now in familiar territory. A linear ODE of the form is solved using an Integrating Factor (I.F.). Here, , so our I.F. is .
Multiplying our ODE by this factor, we get:
Using Integration by Parts, we solve this integral to find . By plugging into the original equation, we find , which forces . Thus, our function is simply .

The Wavy Curve Method

Finally, we turn to . Differentiating this with the Leibniz Rule gives:
Substituting , we get:
Rearranging to keep the terms positive, we have:
The critical points are , , and . By analyzing the signs of these factors, we find that at , the slope changes from negative to positive (a local minimum, ). At , it changes from positive to negative (a local maximum, ). At , the sign does not change because the exponent is even.
The final answer is .

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