(i) LHS = (cosec θ − cot θ)² = ((1 − cos θ)/sin θ)² = (1 − cos θ)²/sin²θ
Replace sin²θ by 1 − cos²θ = (1 − cos θ)(1 + cos θ):
= (1 − cos θ)² / [(1 − cos θ)(1 + cos θ)] = (1 − cos θ)/(1 + cos θ) = RHS ✓
(ii) Put the two fractions over the common denominator cos A(1 + sin A):
LHS = [cos²A + (1 + sin A)²] / [cos A(1 + sin A)]
= [cos²A + 1 + 2 sin A + sin²A] / [cos A(1 + sin A)]
Since cos²A + sin²A = 1, the top is 2 + 2 sin A = 2(1 + sin A):
= 2(1 + sin A)/[cos A(1 + sin A)] = 2/cos A = 2 sec A = RHS ✓
(iii) Write everything in sin and cos. With cot θ = cos θ/sin θ,
first term = (sin θ/cos θ)/((sin θ − cos θ)/sin θ) = sin²θ/[cos θ(sin θ − cos θ)]
second term = (cos θ/sin θ)/((cos θ − sin θ)/cos θ) = cos²θ/[sin θ(cos θ − sin θ)]
The two denominators differ by a sign, so combining over sin θ cos θ (sin θ − cos θ):
= (sin³θ − cos³θ)/[sin θ cos θ(sin θ − cos θ)]
Factor the difference of cubes: sin³θ − cos³θ = (sin θ − cos θ)(sin²θ + sin θ cos θ + cos²θ)
= (sin²θ + sin θ cos θ + cos²θ)/(sin θ cos θ) = (1 + sin θ cos θ)/(sin θ cos θ)
= 1 + 1/(sin θ cos θ) = 1 + sec θ cosec θ = RHS ✓
(iv) LHS = (1 + sec A)/sec A = cos A(1 + sec A) = cos A + 1
RHS = sin²A/(1 − cos A) = (1 − cos²A)/(1 − cos A) = (1 − cos A)(1 + cos A)/(1 − cos A) = 1 + cos A
The two sides agree ✓ — this is the one where working each side separately is much easier than transforming one into the other.
(v) Divide the top and bottom of the LHS by sin A, so that cosec and cot appear:
LHS = (cot A − 1 + cosec A)/(cot A + 1 − cosec A)
Use 1 = cosec²A − cot²A = (cosec A − cot A)(cosec A + cot A) in the numerator:
numerator = (cot A + cosec A) − (cosec A − cot A)(cosec A + cot A)
= (cot A + cosec A)[1 − (cosec A − cot A)]
= (cot A + cosec A)(1 − cosec A + cot A)
The second bracket is exactly the denominator, so it cancels:
= cosec A + cot A = RHS ✓
(vi) Multiply inside the root by (1 + sin A)/(1 + sin A):
LHS = √[(1 + sin A)²/((1 − sin A)(1 + sin A))] = √[(1 + sin A)²/(1 − sin²A)] = √[(1 + sin A)²/cos²A]
= (1 + sin A)/cos A = 1/cos A + sin A/cos A = sec A + tan A = RHS ✓
(vii) Take out the common factors on top and bottom:
LHS = sin θ(1 − 2 sin²θ) / [cos θ(2 cos²θ − 1)]
Now 1 − 2 sin²θ = 1 − 2(1 − cos²θ) = 2 cos²θ − 1, so the two brackets are the same and cancel:
= sin θ/cos θ = tan θ = RHS ✓
(viii) Expand both squares:
(sin A + cosec A)² = sin²A + 2 sin A cosec A + cosec²A = sin²A + 2 + cosec²A
(cos A + sec A)² = cos²A + 2 cos A sec A + sec²A = cos²A + 2 + sec²A
(each middle term is 2, because a ratio times its reciprocal is 1)
Adding: (sin²A + cos²A) + 4 + cosec²A + sec²A = 1 + 4 + (1 + cot²A) + (1 + tan²A)
= 7 + tan²A + cot²A = RHS ✓
(ix) LHS = (1/sin A − sin A)(1/cos A − cos A) = [(1 − sin²A)/sin A][(1 − cos²A)/cos A]
= (cos²A/sin A)(sin²A/cos A) = sin A cos A
RHS = 1/(tan A + cot A) = 1 / [(sin A/cos A) + (cos A/sin A)] = 1 / [(sin²A + cos²A)/(sin A cos A)] = sin A cos A
Both sides equal sin A cos A ✓
(x) Left expression: (1 + tan²A)/(1 + cot²A) = sec²A/cosec²A = sin²A/cos²A = tan²A
Middle expression: rewrite cot A as 1/tan A, so
(1 − tan A)/(1 − 1/tan A) = (1 − tan A) × tan A/(tan A − 1) = −tan A
Squaring gives (−tan A)² = tan²A
So all three expressions equal tan²A ✓
✦ Answer: all ten identities are established.