```latex \text{If } f : (0, \infty) \to \mathbb{R} \text{ be given by}
f(x)=1/xxe(t+1t)dtt. f(x) = \int_{1/x}^{x} e^{-\left(t + \frac{1}{t}\right)} \frac{dt}{t}.
\text{Then,} \begin{itemize} \item[(a)] f(x) \text{ is monotonically increasing on } [1, \infty) \item[(b)] f(x) \text{ is monotonically decreasing on } (0, 1] \item[(c)] f(x) + f\left(\frac{1}{x}\right) = 0, \forall x \in (0, \infty) \item[(d)] f(2^x) \text{ is an odd function of } x \text{ on } \mathbb{R} \end{itemize} ```

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Published July 22, 2025
Calculus
Integral Calculus
Differentiation under Integral Sign
Monotonicity of Functions
Symmetry & Functional Equations

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Detailed Explanation

Key Ideas

  1. Integral with variable limits
    For a function f(x)=a(x)b(x)g(t)dtf(x) = \int_{a(x)}^{b(x)} g(t)\,dt the derivative is f(x)=g(b(x))b(x)    g(a(x))a(x).f'(x) = g\bigl(b(x)\bigr)\,b'(x) \; - \; g\bigl(a(x)\bigr)\,a'(x).

  2. Here

    • (a(x) = 1/x) and (b(x) = x).
    • (g(t) = \dfrac{e^{-(t + 1/t)}}{t}.)
  3. Monotonicity
    If (f'(x) > 0) for the interval of interest, (f) is strictly increasing there.

  4. Symmetry from swapping limits
    Reversing the order of an integral changes its sign: pqg(t)dt=qpg(t)dt.\int_{p}^{q} g(t)\,dt = -\int_{q}^{p} g(t)\,dt. With limits (1/x) and (x), flipping them simply gives (-f(x)).

  5. Oddness through an exponential substitution
    Put (x = 2^u). Then (1/x = 2^{-u}). If (f(2^u) + f(2^{-u}) = 0), the new function (F(u) = f(2^u)) satisfies (F(-u) = -F(u)) — the very definition of an odd function.

Simple Explanation (ELI5)

Imagine a see-saw of arrows

  1. You pick a positive number x.
  2. From 1/x you draw an arrow all the way up to x.
  3. Every short piece of that arrow is weighted by a tiny number (e^{-(t + 1/t)}) (this makes pieces near (t = 1) heavier and far-away pieces lighter).
  4. Add all those tiny weighted pieces – that total is f(x).

Because the same rule is used forward ((1/x \to x)) and backward ((x \to 1/x)), the function behaves like a mirror:

  • Push the right end of the see-saw (make x bigger) and the total weight always goes up – it never dips.
  • Flip the arrow (swap start and end) and you simply get the negative of what you had.

So:

  • From 1 onward the weight only rises.
  • From 1 down to tiny numbers it still rises (just in the opposite direction).
  • The mirror rule gives (f(x) + f(1/x) = 0).
  • Re-label x as (2^x) and the same mirror rule says the graph is an odd curve (symmetric through the origin).

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Step-by-Step Solution

Step-by-Step Solution

  1. Set up the ingredients
    g(t)=e(t+1/t)t,a(x)=1x,b(x)=xg(t) = \frac{e^{-(t + 1/t)}}{t}, \quad a(x) = \frac{1}{x}, \quad b(x) = x

  2. Differentiate using Leibniz rule
    f(x)=g(b(x))b(x)    g(a(x))a(x)f'(x) = g\bigl(b(x)\bigr)\,b'(x) \; - \; g\bigl(a(x)\bigr)\,a'(x) f(x)=g(x)1g ⁣(1x) ⁣(1x2)\Rightarrow f'(x) = g(x) \cdot 1 - g\!\left(\frac{1}{x}\right) \!\left(-\frac{1}{x^{2}}\right) f(x)=g(x)+g(1/x)x2\phantom{f'(x)} = g(x) + \frac{g(1/x)}{x^{2}}

  3. Simplify each term
    g(x)=e(x+1/x)xg(x) = \frac{e^{-(x + 1/x)}}{x} g ⁣(1x)=e(1/x+x)1/x=xe(x+1/x)g\!\left(\frac{1}{x}\right) = \frac{e^{-(1/x + x)}}{1/x} = x\,e^{-(x + 1/x)} Hence g(1/x)x2=xe(x+1/x)x2=e(x+1/x)x\frac{g(1/x)}{x^{2}} = \frac{x\,e^{-(x + 1/x)}}{x^{2}} = \frac{e^{-(x + 1/x)}}{x}

  4. Add them up
    f(x)=e(x+1/x)x+e(x+1/x)x=2e(x+1/x)xf'(x) = \frac{e^{-(x + 1/x)}}{x} + \frac{e^{-(x + 1/x)}}{x} = \frac{2\,e^{-(x + 1/x)}}{x}

  5. Sign of the derivative
    For every (x>0): (e^{-(x + 1/x)} > 0) and (x > 0). Therefore f(x)>0x>0.f'(x) > 0 \quad \forall\,x>0. So (f) is strictly increasing everywhere on ((0,\infty)).

    • (a) True on ([1,\infty)).
    • (b) False (because it increases, not decreases, on ((0,1])).

  6. Reciprocal relation
    (f(1/x) = \int_{x}^{1/x} g(t),dt = -\int_{1/x}^{x} g(t),dt = -f(x)).
    So f(x)+f ⁣(1x)=0f(x) + f\!\left(\frac{1}{x}\right) = 0 making statement (c) True.

  7. Oddness after substitution
    Let (F(u) = f(2^{u})). Then F(u)=f(2u)=f ⁣(12u)=f(2u)=F(u).F(-u) = f(2^{-u}) = f\!\left(\frac{1}{2^{u}}\right) = -f(2^{u}) = -F(u). Therefore (F) is an odd function of (u), verifying statement (d) True.

[\boxed{\text{Correct options: (a), (c), (d)}}]

Examples

Example 1

Growth/decay models where integrating from 1/x to x captures equal percentage bands around 1

Example 2

Optics problems involving lens formulas where reciprocals arise naturally (object distance vs. image distance)

Example 3

Thermodynamic identities using variables T and 1/T to express symmetry in partition functions

Visual Representation

References

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