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JEE Advanced 1987
LEVELJEE Main

Animated Solution for Mathematics - Trigonometry: The number of all possible triplets such that for all is

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Visualized Solution

The Given Equation

  • Given Equation:
  • Condition: Valid for all
  • This means it is an identity, not just an equation to solve for .

Identifying the Mismatch

  • We have two different trigonometric functions: and .
  • To compare terms, we must convert them into a single function.

The Double Angle Identity

  • Recall the double angle formula for cosine.
  • This perfectly links our two terms.

Substituting the Identity

  • Substitute with .

Expanding the Bracket

  • Distribute into the bracket.

Grouping Like Terms

  • Group the constant terms:
  • Group the terms:
  • Combined:

The Principle of Identity

  • We have an equation of the form .
  • Since it holds for all , the functions and are linearly independent.
  • Therefore, their coefficients must individually be zero: and .

Equating the Constant Term to Zero

  • Set the constant part to zero.
  • This gives .

Equating the Coefficient to Zero

  • Set the coefficient of to zero.
  • This gives .

Forming the General Triplet

  • Let , where .
  • Then and .
  • The triplet becomes .

Final Conclusion

  • The parameter can be any real number.
  • For every choice of , we get a valid triplet.
  • Therefore, there are infinitely many such triplets.
  • Final Answer: infinite

The Sigma Insight: Trigonometric Ratios and Identities

Solution Diagram

Analyzing the Setup

Imagine you are standing before a mathematical puzzle that seems to defy simple logic. You are given the equation and told it must hold for all .
At first glance, your instinct might be to solve for . But stop! The phrase "for all " is the most powerful sentence in this problem.
It transforms the equation from a simple puzzle into a profound statement of identity. We are not looking for a specific ; we are looking for the hidden structure that makes this expression vanish regardless of the input.

The Art of Translation

To solve this, we must first recognize that our terms are speaking different languages. We have a and a .
They are like two people trying to communicate in different dialects. To make sense of the identity, we must bring them onto common ground.
This is where the double-angle identity for cosine comes to our rescue:
This formula is the bridge that connects our two terms. By substituting this into our original equation, we replace the cosine term with something that speaks the language of .

The Algebraic Cleanup

Let's perform the substitution:
Now, we distribute the term. It is crucial to be careful with the signs here—a small slip could derail the entire process. We get:
Now, let's group the terms. We have the constant part, , and the part dependent on , which is . Our equation now looks like this:

The Principle of Linear Independence

Here is the core of the problem. We have an expression of the form . For this to be true for every single value of , the coefficients and must independently be zero.
Why? Because and are linearly independent functions. They do not "cancel each other out" unless their individual coefficients are zero.
So, we set the constant part to zero:
Then, we set the coefficient of to zero:

The Infinite Possibilities

We have successfully expressed and in terms of . Let's introduce a parameter such that . Then, our triplet becomes .
Think about what this means. For any real number you choose—be it or even —you will generate a valid triplet that satisfies the original equation.
Because can be any real number, there are infinitely many such triplets. This is the elegance of the identity: it doesn't restrict us to a single answer; it reveals an entire family of solutions, all bound by the same beautiful mathematical law.

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