Animated Solution for Mathematics - Trigonometry: General value of θ satisfying the equation tan2θ+sec2θ=1 is ..........
Visualized Solution
Introduction to the Equation
Given equation: tan2θ+sec2θ=1
Goal: Express the entire equation in terms of tanθ.
Applying the Double Angle Identity
Recall the identity: cos2θ=1+tan2θ1−tan2θ
Expressing sec2θ
Therefore: sec2θ=cos2θ1=1−tan2θ1+tan2θ
Substituting into the Equation
Substitute the identity into the original equation:
tan2θ+1−tan2θ1+tan2θ=1
Clearing the Denominator
Multiply the entire equation by (1−tan2θ):
tan2θ(1−tan2θ)+(1+tan2θ)=1−tan2θ
Expanding and Simplifying
Expand the terms: tan2θ−tan4θ+1+tan2θ=1−tan2θ
Simplify by canceling 1 and rearranging: 3tan2θ−tan4θ=0
Factoring the Equation
Factor out tan2θ:
tan2θ(3−tan2θ)=0
This gives two cases: tan2θ=0 or 3−tan2θ=0
Case 1: Solving for tanθ=0
Case 1: tan2θ=0⇒tanθ=0
General solution: θ=nπ, where n∈Z
Case 2: Solving for tan2θ=3
Case 2: 3−tan2θ=0⇒tan2θ=3
We know tan2(3π)=(3)2=3
General solution for tan2θ=tan2α is θ=nπ±α
So, θ=nπ±3π
Final Conclusion and Summary
Final general values of θ:
θ=nπ and θ=nπ±3π
Where n is any integer (n∈Z).
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The Sigma Insight: General Solution of Trigonometric Equations
Solution Diagram
Analyzing the Setup
Welcome, fellow traveler on the path to JEE mastery! Today, we are not just solving a trigonometric equation; we are embarking on a journey of simplification and elegance.
When you look at the equation tan2θ+sec2θ=1, it might seem like a chaotic mess of different functions and angles. But remember, in mathematics, chaos is often just order waiting to be discovered.
Our mission is to bring harmony to this equation by unifying everything into a single language: the language of tanθ.
The Bridge of Identities
The primary obstacle here is the mismatch between θ and 2θ. We cannot easily combine terms when they are speaking different languages. We need a bridge.
That bridge is the double-angle identity for cosine:
cos2θ=1+tan2θ1−tan2θ
This identity is a masterpiece of trigonometry, allowing us to leap from the double angle 2θ back to the single angle θ. Since we have sec2θ in our equation, we simply take the reciprocal of this identity:
sec2θ=1−tan2θ1+tan2θ
The Algebraic Dance
With our identity in hand, we substitute it back into the original equation:
tan2θ+1−tan2θ1+tan2θ=1
We can clear the path by multiplying the entire equation by the denominator, (1−tan2θ). This yields:
tan2θ(1−tan2θ)+(1+tan2θ)=1−tan2θ
Expanding this, we get:
tan2θ−tan4θ+1+tan2θ=1−tan2θ
Notice the magic happening here? The 1 on both sides cancels out beautifully, leaving us with:
2tan2θ−tan4θ=−tan2θ
Rearranging this, we arrive at the elegant form:
3tan2θ−tan4θ=0
The Bifurcation of Solutions
We have arrived at the climax of our journey. Factoring out tan2θ, we get:
tan2θ(3−tan2θ)=0
This splits our problem into two distinct, manageable cases.
Case 1:tan2θ=0, which implies tanθ=0. On the unit circle, this occurs at every integer multiple of π, so θ=nπ.
Case 2:3−tan2θ=0, which means tan2θ=3. We know that tan(3π)=3, so tan2(3π)=3.
The general solution for tan2θ=tan2α is θ=nπ±α. Substituting α=3π, we get θ=nπ±3π.
Final Harmony
By combining these two cases, we reach our final destination. The general solution is:
θ=nπ and θ=nπ±3π
(where n is any integer). We have successfully navigated the complexity, cleared the denominators, and found the hidden symmetry. Remember, every time you face a daunting equation, look for the identity that bridges the gap.