Animated Solution for Mathematics - Differentiation: Let f(x)=sinx−cosxsinx+cosx−2,x∈[0,π]−{4π}, then f(127π)f′′(127π) is equal to
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Visualized Solution
Analyze the Function f(x)
Given function: f(x)=sinx−cosxsinx+cosx−2
Domain: x∈[0,π]∖{4π}
Goal: Find f(127π)⋅f′′(127π)
Simplify the Numerator
Numerator: sinx+cosx−2
Use identity: sinx+cosx=2sin(x+4π)
Factored: 2(sin(x+4π)−1)
Simplify the Denominator
Denominator: sinx−cosx
Use identity: sinx−cosx=2sin(x−4π)
Combine and Substitute
f(x)=2sin(x−4π)2(sin(x+4π)−1)
f(x)=sin(x−4π)sin(x+4π)−1
Variable Substitution
Let u=x−4π⟹x+4π=u+2π
f(x)=sinusin(u+2π)−1
f(x)=sinucosu−1
Apply Half-Angle Identity
Identity: cosu−1=−2sin2(2u)
Identity: sinu=2sin(2u)cos(2u)
f(x)=2sin(u/2)cos(u/2)−2sin2(u/2)=−tan(2u)
Final Form of f(x)
Substitute u=x−4π back:
f(x)=−tan(2x−π/4)
f(x)=−tan(2x−8π)
First Derivative f′(x)
Differentiate f(x)=−tan(2x−8π)
f′(x)=−sec2(2x−8π)⋅dxd(2x−8π)
f′(x)=−21sec2(2x−8π)
Second Derivative f′′(x)
f′′(x)=−21⋅2sec(2x−8π)⋅dxd(sec(2x−8π))
f′′(x)=−sec(2x−8π)⋅sec(2x−8π)tan(2x−8π)⋅21
f′′(x)=−21sec2(2x−8π)tan(2x−8π)
Evaluate Angle at x=127π
Let's find the angle θ=2x−8π at x=127π
θ=247π−8π
θ=247π−3π=244π=6π
Evaluate f(127π)
Recall: f(x)=−tan(2x−8π)
Substitute angle 6π:
f(127π)=−tan(6π)=−31
Evaluate f′′(127π)
Recall: f′′(x)=−21sec2(θ)tan(θ)
sec(6π)=32⟹sec2(6π)=34
f′′(127π)=−21⋅(34)⋅(31)=−332
Final Calculation
Product: f(127π)⋅f′′(127π)
=(−31)⋅(−332)
=3⋅32=92
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The Sigma Insight: Higher Order Derivatives
Solution Diagram
The Art of Mathematical Simplification
Imagine you are standing at the base of a massive, jagged mountain. The problem before us, f(x)=sinx−cosxsinx+cosx−2, is that mountain.
If you try to climb it by brute-forcing the quotient rule, you will find yourself exhausted, tangled in a web of derivatives, and likely lost in a sea of algebraic errors. But what if there was a hidden path, a secret trail that leads straight to the summit? That is what we are going to find today.
Phase 1
The R-Method
Our first step is to look at the numerator and denominator not as a chaotic mess, but as structured trigonometric entities. We know that any expression of the form asinx+bcosx can be condensed into a single sine wave.
By multiplying and dividing by a2+b2, we can rewrite sinx+cosx as 2sin(x+4π) and sinx−cosx as 2sin(x−4π).
Suddenly, the mountain doesn't look so steep. Our function becomes:
f(x)=2sin(x−4π)2(sin(x+4π)−1)
The 2 terms cancel out, leaving us with a much cleaner expression. But we can do better.
Phase 2
The Elegant Substitution
To truly simplify, we need to tame the arguments. Let us introduce a new variable, u=x−4π. This implies x+4π=u+2π.
Substituting this into our function, we get:
f(x)=sinusin(u+2π)−1
Using the allied angle identity sin(u+2π)=cosu, our function transforms into the beautiful, compact form:
f(x)=sinucosu−1
Phase 3
The Half-Angle Magic
Now, we reach the most satisfying part of the journey. We use the half-angle identities: cosu−1=−2sin2(2u) and sinu=2sin(2u)cos(2u).
When we divide these, the terms cancel with surgical precision:
f(x)=2sin(2u)cos(2u)−2sin2(2u)=−tan(2u)
Substituting u=x−4π back in, we find our final, simplified function: f(x)=−tan(2x−8π).
Phase 4
The Calculus Sprint
Now that we have a simple tangent function, differentiation is a breeze. The first derivative is f′(x)=−21sec2(2x−8π).
Differentiating again, we apply the chain rule to get: