Analyzing the Setup
Welcome, fellow explorer of the mathematical universe! Today, we are going to dissect a problem that at first glance might seem like a chaotic mess of constraints, but as we peel back the layers, it reveals a structure of pure, crystalline elegance.
We are dealing with a twice-differentiable function
f:R→[−2,2] with a peculiar condition at the origin:
(f(0))2+(f′(0))2=85
Phase 1
The Constraint at the Origin
First, let's ground ourselves. We are given that f(x) is trapped within the interval [−2,2], which implies that for any x, ∣f(x)∣≤2. Consequently, at x=0, we must have (f(0))2≤4.
Now, look at our given constraint:
(f(0))2+(f′(0))2=85. If we isolate the derivative term, we get:
(f′(0))2=85−(f(0))2
Since (f(0))2 is at most 4, the derivative squared must be at least 85−4=81. This implies ∣f′(0)∣≥9.
This is an incredibly steep tangent! This immediately tells us that $f'(0)
e 0$. Because the function is twice differentiable, the derivative is continuous, meaning the slope will maintain its sign in a small neighborhood around zero.
A function with a non-zero derivative in an interval is strictly monotonic, and thus, one-one. Option A is confirmed true.
Phase 2
The MVT Insight
Now, let's tackle Option B. We need to find a point x0∈(−4,0) such that ∣f′(x0)∣≤1.
This is a classic setup for the Lagrange Mean Value Theorem (L.M.V.T.). Let's apply it on the interval
[−4,0]. The theorem guarantees the existence of a point
x0 such that:
f′(x0)=0−(−4)f(0)−f(−4)
The magnitude of this slope is 4∣f(0)−f(−4)∣. By the triangle inequality, ∣f(0)−f(−4)∣≤∣f(0)∣+∣f(−4)∣≤2+2=4.
Thus, ∣f′(x0)∣≤44=1. The logic is airtight. Option B is also true.
Phase 3
The Auxiliary Function Masterstroke
Finally, we arrive at the most thrilling part: Option D. We need to find α∈(−4,4) such that f(α)+f′′(α)=0.
This looks like a differential equation, but it's actually a hint to construct an auxiliary function. Let's define g(x)=(f(x))2+(f′(x))2. We know g(0)=85.
Using the same MVT logic we used for Option B, we can find points
x0∈(−4,0) and
x1∈(0,4) where
∣f′(x0)∣≤1 and
∣f′(x1)∣≤1. At these points:
g(x0)=(f(x0))2+(f′(x0))2≤22+12=5
g(x1)=(f(x1))2+(f′(x1))2≤22+12=5
So, g(x) starts at a value ≤5 at x0, climbs to 85 at x=0, and drops back to ≤5 at x1. By the Extreme Value Theorem, g(x) must attain a local maximum at some point α between x0 and x1.
At this local maximum,
g′(α)=0. Let's differentiate
g(x):
g′(x)=2f(x)f′(x)+2f′(x)f′′(x)=2f′(x)[f(x)+f′′(x)]
Setting this to zero at
α, we get:
2f′(α)[f(α)+f′′(α)]=0
We already proved that f′(α) cannot be zero because g(α)≥85. Therefore, the only possibility is f(α)+f′′(α)=0.
And there it is! The elegance of calculus in action. We have navigated the constraints, applied the fundamental theorems, and arrived at the truth. Option D is true.