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Class 10Trigonometry13:08Published 12 Sept 2025

Trigonometric Identity Proofs (Exercise 8.3, Part 2)

Worked proofs from Exercise 8.3 of the Class 10 trigonometry chapter, showing how to prove identities by simplifying one side until it matches the other.

This lesson works through four identity proofs from Exercise 8.3. It starts with rationalising a square-root expression, then expands squares of sums, and handles a three-part identity by proving each piece equals a common result. The final, longer proof combines two fractions and uses the sum-of-cubes factorisation to reach the answer.

What you'll learn

  • How to prove a trig identity by simplifying one side until it matches the other
  • Rationalising a fraction under a square root using the conjugate of the denominator
  • Expanding squares of sums and collecting terms with the Pythagorean identities
  • Proving a three-part identity by showing each expression equals a common value

Lesson chapters

0:00Three ways to prove an identity
0:46Rationalising to prove sec a + tan a
2:40Expanding squares of sums
4:35A three-part identity equal to tan squared
7:27Combining two fractions with sum of cubes
11:48Second approach: one over tan plus cot

Lesson notes

This lesson works through four proofs from Exercise 8.3 of the Class 10 trigonometry chapter. An identity can be proved by simplifying the left side down to the right, the right side down to the left, or by reducing both sides to a common expression.

Proving 1+sin⁡a1−sin⁡a=sec⁡a+tan⁡a\sqrt{\tfrac{1+\sin a}{1-\sin a}} = \sec a + \tan a

Start from the left side and rationalise by multiplying numerator and denominator inside the root by the conjugate of the denominator, 1+sin⁡a1 + \sin a.

1+sin⁡a1−sin⁡a=(1+sin⁡a)(1+sin⁡a)(1−sin⁡a)(1+sin⁡a)=(1+sin⁡a)21−sin⁡2a\sqrt{\frac{1+\sin a}{1-\sin a}} = \sqrt{\frac{(1+\sin a)(1+\sin a)}{(1-\sin a)(1+\sin a)}} = \sqrt{\frac{(1+\sin a)^2}{1-\sin^2 a}}

Since 1−sin⁡2a=cos⁡2a1 - \sin^2 a = \cos^2 a, the root simplifies cleanly.

(1+sin⁡a)2cos⁡2a=1+sin⁡acos⁡a=1cos⁡a+sin⁡acos⁡a=sec⁡a+tan⁡a\sqrt{\frac{(1+\sin a)^2}{\cos^2 a}} = \frac{1+\sin a}{\cos a} = \frac{1}{\cos a} + \frac{\sin a}{\cos a} = \sec a + \tan a

This equals the right side.

Proving (sin⁡a+csc⁡a)2+(cos⁡a+sec⁡a)2=7+tan⁡2a+cot⁡2a(\sin a + \csc a)^2 + (\cos a + \sec a)^2 = 7 + \tan^2 a + \cot^2 a

Take the left side and expand each bracket with (x+y)2=x2+2xy+y2(x+y)^2 = x^2 + 2xy + y^2.

sin⁡2a+csc⁡2a+2sin⁡a csc⁡a+cos⁡2a+sec⁡2a+2cos⁡a sec⁡a\sin^2 a + \csc^2 a + 2\sin a\,\csc a + \cos^2 a + \sec^2 a + 2\cos a\,\sec a

Here sin⁡a csc⁡a=1\sin a\,\csc a = 1 and cos⁡a sec⁡a=1\cos a\,\sec a = 1, and sin⁡2a+cos⁡2a=1\sin^2 a + \cos^2 a = 1.

1+csc⁡2a+sec⁡2a+2+21 + \csc^2 a + \sec^2 a + 2 + 2

Now replace csc⁡2a=1+cot⁡2a\csc^2 a = 1 + \cot^2 a and sec⁡2a=1+tan⁡2a\sec^2 a = 1 + \tan^2 a to bring in the terms needed on the right.

1+(1+cot⁡2a)+(1+tan⁡2a)+4=7+tan⁡2a+cot⁡2a1 + (1 + \cot^2 a) + (1 + \tan^2 a) + 4 = 7 + \tan^2 a + \cot^2 a

This equals the right side.

Proving 1+tan⁡2a1+cot⁡2a=(1−tan⁡a1−cot⁡a)2=tan⁡2a\dfrac{1+\tan^2 a}{1+\cot^2 a} = \left(\dfrac{1-\tan a}{1-\cot a}\right)^2 = \tan^2 a

With three expressions, prove the first equals the last, then the middle equals the last; if both equal tan⁡2a\tan^2 a, all three are equal.

First expression equals the last

1+tan⁡2a1+cot⁡2a=sec⁡2acsc⁡2a=1/cos⁡2a1/sin⁡2a=sin⁡2acos⁡2a=tan⁡2a\frac{1+\tan^2 a}{1+\cot^2 a} = \frac{\sec^2 a}{\csc^2 a} = \frac{1/\cos^2 a}{1/\sin^2 a} = \frac{\sin^2 a}{\cos^2 a} = \tan^2 a

Middle expression equals the last

Replace cot⁡a=1tan⁡a\cot a = \tfrac{1}{\tan a} and take the LCM in the denominator.

(1−tan⁡a1−cot⁡a)2=(1−tan⁡a)2(tan⁡a−1tan⁡a)2=(1−tan⁡a)2 tan⁡2a(tan⁡a−1)2\left(\frac{1-\tan a}{1-\cot a}\right)^2 = \frac{(1-\tan a)^2}{\left(\frac{\tan a - 1}{\tan a}\right)^2} = \frac{(1-\tan a)^2\,\tan^2 a}{(\tan a - 1)^2}

Since (1−tan⁡a)2=(tan⁡a−1)2(1-\tan a)^2 = (\tan a - 1)^2, those factors cancel.

=tan⁡2a= \tan^2 a

Both pieces equal tan⁡2a\tan^2 a, so all three expressions are equal.

Proving tan⁡θ1−cot⁡θ+cot⁡θ1−tan⁡θ=1+sec⁡θ csc⁡θ\dfrac{\tan\theta}{1-\cot\theta} + \dfrac{\cot\theta}{1-\tan\theta} = 1 + \sec\theta\,\csc\theta

Write tan⁡θ\tan\theta and cot⁡θ\cot\theta in terms of sine and cosine, then simplify each denominator with an LCM.

sin⁡θcos⁡θ1−cos⁡θsin⁡θ+cos⁡θsin⁡θ1−sin⁡θcos⁡θ=sin⁡2θcos⁡θ(sin⁡θ−cos⁡θ)+cos⁡2θsin⁡θ(cos⁡θ−sin⁡θ)\frac{\frac{\sin\theta}{\cos\theta}}{1-\frac{\cos\theta}{\sin\theta}} + \frac{\frac{\cos\theta}{\sin\theta}}{1-\frac{\sin\theta}{\cos\theta}} = \frac{\sin^2\theta}{\cos\theta(\sin\theta-\cos\theta)} + \frac{\cos^2\theta}{\sin\theta(\cos\theta-\sin\theta)}

Take a negative sign out of the second denominator so both brackets read sin⁡θ−cos⁡θ\sin\theta - \cos\theta, then factor it out.

1sin⁡θ−cos⁡θ(sin⁡2θcos⁡θ−cos⁡2θsin⁡θ)=1sin⁡θ−cos⁡θ⋅sin⁡3θ−cos⁡3θsin⁡θcos⁡θ\frac{1}{\sin\theta-\cos\theta}\left(\frac{\sin^2\theta}{\cos\theta} - \frac{\cos^2\theta}{\sin\theta}\right) = \frac{1}{\sin\theta-\cos\theta}\cdot\frac{\sin^3\theta-\cos^3\theta}{\sin\theta\cos\theta}

The numerator is a difference of cubes, a3−b3=(a−b)(a2+ab+b2)a^3 - b^3 = (a-b)(a^2+ab+b^2).

=1sin⁡θ−cos⁡θ⋅(sin⁡θ−cos⁡θ)(sin⁡2θ+sin⁡θcos⁡θ+cos⁡2θ)sin⁡θcos⁡θ= \frac{1}{\sin\theta-\cos\theta}\cdot\frac{(\sin\theta-\cos\theta)(\sin^2\theta+\sin\theta\cos\theta+\cos^2\theta)}{\sin\theta\cos\theta}

Cancel sin⁡θ−cos⁡θ\sin\theta - \cos\theta, and use sin⁡2θ+cos⁡2θ=1\sin^2\theta+\cos^2\theta = 1.

=1+sin⁡θcos⁡θsin⁡θcos⁡θ=1sin⁡θcos⁡θ+1=1+sec⁡θ csc⁡θ= \frac{1+\sin\theta\cos\theta}{\sin\theta\cos\theta} = \frac{1}{\sin\theta\cos\theta} + 1 = 1 + \sec\theta\,\csc\theta

This equals the right side.

A second approach to a related result

The expression 1tan⁡a+cot⁡a\dfrac{1}{\tan a + \cot a} can also be simplified directly.

1tan⁡a+cot⁡a=1sin⁡acos⁡a+cos⁡asin⁡a=sin⁡acos⁡asin⁡2a+cos⁡2a=sin⁡acos⁡a1=sin⁡acos⁡a\frac{1}{\tan a + \cot a} = \frac{1}{\frac{\sin a}{\cos a} + \frac{\cos a}{\sin a}} = \frac{\sin a\cos a}{\sin^2 a + \cos^2 a} = \frac{\sin a\cos a}{1} = \sin a\cos a

Key takeaways

  • Rationalising a fraction under a root with the conjugate turns 1−sin⁡2a1 - \sin^2 a into cos⁡2a\cos^2 a.
  • After expanding, use sin⁡a csc⁡a=1\sin a\,\csc a = 1, cos⁡a sec⁡a=1\cos a\,\sec a = 1, csc⁡2a=1+cot⁡2a\csc^2 a = 1 + \cot^2 a, and sec⁡2a=1+tan⁡2a\sec^2 a = 1 + \tan^2 a.
  • A three-part identity is proved by showing each expression reduces to the same value.
  • Factoring out a common denominator and applying the difference of cubes simplifies the combined fraction to 1+sec⁡θ csc⁡θ1 + \sec\theta\,\csc\theta.