Animated Solution for Mathematics - Differentiation: Let f be a twice differentiable function such that f′′(x)=−f(x), and f′(x)=g(x),h(x)=[f(x)]2+[g(x)]2. Find h(10) if h(5)=11.
Enter Numerical Value:
Visualized Solution
The Given Functions
Given: f′′(x)=−f(x)
Given: f′(x)=g(x)
Define: h(x)=[f(x)]2+[g(x)]2
Analyzing h(x)
Goal: Find h(10) given h(5)=11.
Strategy: Determine how h(x) changes with x.
Geometrically, h(x) is the distance from the origin to (f(x),g(x)).
Differentiating h(x)
To find the rate of change, differentiate h(x) with respect to x.
h′(x)=dxd([f(x)]2+[g(x)]2)
Applying the Chain Rule
Differentiate using the Chain Rule:
dxd[f(x)]2=2f(x)f′(x)
dxd[g(x)]2=2g(x)g′(x)
h′(x)=2f(x)f′(x)+2g(x)g′(x)
Using Given Relations
We are given: f′(x)=g(x)
We need an expression for g′(x) to substitute into h′(x).
Finding g′(x)
Start with: f′(x)=g(x)
Differentiate both sides with respect to x:
f′′(x)=g′(x)
Substituting f′′(x)
We are given: f′′(x)=−f(x)
Therefore, g′(x)=−f(x)
Substituting into h′(x)
Recall: h′(x)=2f(x)f′(x)+2g(x)g′(x)
Substitute f′(x)=g(x) and g′(x)=−f(x):
h′(x)=2f(x)[g(x)]+2g(x)[−f(x)]
The Vanishing Derivative
Simplify the expression:
h′(x)=2f(x)g(x)−2f(x)g(x)
h′(x)=0
Constant Function
Since h′(x)=0 for all x, h(x) does not change.
Therefore, h(x)=C (a constant function).
The point (f(x),g(x)) moves on a circle of radius C.
Final Evaluation
We know h(x)=C.
Given initial condition: h(5)=11.
So, C=11, which means h(x)=11 for all x.
Therefore, h(10)=11.
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The Sigma Insight: Higher Order Derivatives
Solution Diagram
The Hidden Symmetry of Motion
Imagine you are standing at the edge of a vast, tranquil lake. You throw a stone, and the ripples spread out in perfect, concentric circles.
In mathematics, we often encounter functions that seem complex at first glance, yet they possess a hidden, underlying symmetry that keeps them perfectly balanced. Today, we are going to explore one such problem—a problem that initially looks like a daunting task of calculus but reveals itself to be a beautiful demonstration of conservation.
The Setup
Defining Our Players
We are given a twice-differentiable function f(x) that satisfies the elegant differential equation f′′(x)=−f(x). This is the signature equation of Simple Harmonic Motion, the heartbeat of the physical universe.
We are also given a secondary function g(x)=f′(x), and a composite function h(x)=[f(x)]2+[g(x)]2. Our mission is to find h(10) given that h(5)=11.
At first, you might be tempted to solve for f(x) directly. You might think, "I need to find the exact form of f(x) to plug in x=10."
But hold that thought. In the world of JEE Advanced, the most elegant path is rarely the one that requires the most brute force. Instead, let us ask a more profound question: How does h(x) behave as x changes?
The Calculus of Change
To understand the behavior of h(x), we must look at its rate of change. We differentiate h(x) with respect to x using the chain rule:
h′(x)=dxd([f(x)]2+[g(x)]2)=2f(x)f′(x)+2g(x)g′(x)
This expression is the key to the entire problem. We know f′(x)=g(x).
But what about g′(x)? Since g(x)=f′(x), it follows that g′(x)=f′′(x). And here is where the magic happens: we are given that f′′(x)=−f(x). Therefore, g′(x)=−f(x).
The Vanishing Derivative
Now, let us substitute these pieces back into our derivative equation. Watch closely as the terms interact:
h′(x)=2f(x)[g(x)]+2g(x)[−f(x)]
Look at that! We have 2f(x)g(x)−2f(x)g(x). The terms cancel out perfectly, leaving us with h′(x)=0.
This is a monumental realization. If the derivative of a function is zero everywhere, the function itself must be a constant. It does not matter if x is 5, 10, or 100; the value of h(x) remains locked in time.
The Final Revelation
Because h(x) is a constant, we can say h(x)=C. We were given the initial condition h(5)=11.
This tells us that our constant C is exactly 11. Since the function never changes, it must be true that h(10)=11.
Think about what this means geometrically. The point (f(x),g(x)) is tracing a circle in the Cartesian plane. As x increases, the point moves along the circumference, but its distance from the origin—represented by h(x)—remains perfectly fixed.
You have just solved a problem that describes the conservation of energy in a harmonic system. You didn't just calculate a number; you uncovered a fundamental truth about the system. Keep this perspective, and you will find that even the most intimidating JEE problems are just stories waiting to be told.