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Class 10Trigonometry4:32Published 3 Dec 2025

Trigonometry Proof: Expression Independent of Theta

A class 10 trigonometry proof showing that a sum of three trigonometric terms simplifies to the constant 13, completely independent of the angle theta.

This lesson works through an important class 10 trigonometry question. Starting from an expression built from powers of sine and cosine, the teacher expands every term with standard algebraic identities and the Pythagorean identity. After substitution and cancellation, all the angle-dependent parts disappear and the whole expression collapses to the constant 13, proving it does not depend on theta.

What you'll learn

  • How to expand squared and fourth-power binomials of sine and cosine
  • How to simplify the sum of sixth powers using the sum of cubes identity
  • How using the Pythagorean identity makes the angle terms cancel to leave a constant

Lesson chapters

0:00The question to prove
0:24Rewriting each term as squares and cubes
1:08Expanding with the binomial identities
2:15Applying the Pythagorean identity
3:29Cancelling terms to reach 13

Lesson notes

This lesson proves an important class 10 trigonometry result: that the expression below has the same value for every angle θ\theta. We expand each term with algebraic identities, use sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1, and watch the angle-dependent parts cancel.

The expression to evaluate

We want to show that

3(sin⁡θ−cos⁡θ)4+6(sin⁡θ+cos⁡θ)2+4(sin⁡6θ+cos⁡6θ)3(\sin\theta - \cos\theta)^4 + 6(\sin\theta + \cos\theta)^2 + 4(\sin^6\theta + \cos^6\theta)

is independent of θ\theta.

Rewriting each term

We first rewrite the powers so we can apply standard identities:

  • (sin⁡θ−cos⁡θ)4=[(sin⁡θ−cos⁡θ)2]2(\sin\theta - \cos\theta)^4 = \big[(\sin\theta - \cos\theta)^2\big]^2
  • sin⁡6θ+cos⁡6θ=(sin⁡2θ)3+(cos⁡2θ)3\sin^6\theta + \cos^6\theta = (\sin^2\theta)^3 + (\cos^2\theta)^3, a sum of cubes.

First term

Using (a−b)2=a2−2ab+b2(a - b)^2 = a^2 - 2ab + b^2 with the Pythagorean identity sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1:

(sin⁡θ−cos⁡θ)2=1−2sin⁡θcos⁡θ(\sin\theta - \cos\theta)^2 = 1 - 2\sin\theta\cos\theta

Squaring again,

(sin⁡θ−cos⁡θ)4=(1−2sin⁡θcos⁡θ)2=1−4sin⁡θcos⁡θ+4sin⁡2θcos⁡2θ(\sin\theta - \cos\theta)^4 = (1 - 2\sin\theta\cos\theta)^2 = 1 - 4\sin\theta\cos\theta + 4\sin^2\theta\cos^2\theta

Multiplying by 33:

3(sin⁡θ−cos⁡θ)4=3−12sin⁡θcos⁡θ+12sin⁡2θcos⁡2θ3(\sin\theta - \cos\theta)^4 = 3 - 12\sin\theta\cos\theta + 12\sin^2\theta\cos^2\theta

Second term

Using (a+b)2=a2+2ab+b2(a + b)^2 = a^2 + 2ab + b^2:

(sin⁡θ+cos⁡θ)2=1+2sin⁡θcos⁡θ(\sin\theta + \cos\theta)^2 = 1 + 2\sin\theta\cos\theta

Multiplying by 66:

6(sin⁡θ+cos⁡θ)2=6+12sin⁡θcos⁡θ6(\sin\theta + \cos\theta)^2 = 6 + 12\sin\theta\cos\theta

Third term

Using the sum of cubes a3+b3=(a+b)3−3ab(a+b)a^3 + b^3 = (a + b)^3 - 3ab(a + b) with a=sin⁡2θa = \sin^2\theta, b=cos⁡2θb = \cos^2\theta, so that a+b=1a + b = 1:

sin⁡6θ+cos⁡6θ=13−3sin⁡2θcos⁡2θ⋅1=1−3sin⁡2θcos⁡2θ\sin^6\theta + \cos^6\theta = 1^3 - 3\sin^2\theta\cos^2\theta \cdot 1 = 1 - 3\sin^2\theta\cos^2\theta

Multiplying by 44:

4(sin⁡6θ+cos⁡6θ)=4−12sin⁡2θcos⁡2θ4(\sin^6\theta + \cos^6\theta) = 4 - 12\sin^2\theta\cos^2\theta

Adding everything together

Lining up the three expanded terms:

(3−12sin⁡θcos⁡θ+12sin⁡2θcos⁡2θ)+(6+12sin⁡θcos⁡θ)+(4−12sin⁡2θcos⁡2θ)\big(3 - 12\sin\theta\cos\theta + 12\sin^2\theta\cos^2\theta\big) + \big(6 + 12\sin\theta\cos\theta\big) + \big(4 - 12\sin^2\theta\cos^2\theta\big)

The sin⁡θcos⁡θ\sin\theta\cos\theta terms cancel (−12-12 and +12+12), and the sin⁡2θcos⁡2θ\sin^2\theta\cos^2\theta terms cancel (+12+12 and −12-12). Only the constants remain:

3+6+4=133 + 6 + 4 = 13

Since no θ\theta survives, the value is always 1313.

Key takeaways

  • (sin⁡θ±cos⁡θ)2=1±2sin⁡θcos⁡θ(\sin\theta \pm \cos\theta)^2 = 1 \pm 2\sin\theta\cos\theta, straight from the Pythagorean identity.
  • sin⁡6θ+cos⁡6θ=1−3sin⁡2θcos⁡2θ\sin^6\theta + \cos^6\theta = 1 - 3\sin^2\theta\cos^2\theta via the sum of cubes.
  • After expansion, every angle-dependent term cancels, leaving the constant 1313, so the expression is independent of θ\theta.