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The Trigonometric identities are fundamental formulas in trigonometry that relate the angles and sides of the triangles. These identities simplify trigonometric expressions and solve the equations involving trigonometric functions. In Class 10 RD Sharma's Chapter 6 on the Trigonometric Identities Exercise 6.1 | Set 3 provides practice problems to the reinforce these concepts and apply them effectively.
The Trigonometric identities are equations involving the trigonometric functions that hold for all angles. Here are four key trigonometric identities:
This identity arises from the Pythagorean theorem applied to the unit circle.
These identities express the reciprocal relationships between the trigonometric functions.
These identities define the tangent and cotangent functions in terms of the sine and cosine.
These identities relate the sine and cosine of the complementary angles.
Solution:
We have,
L.H.S. = tan2 A sec2 B − sec2 A tan2 B
= tan2 A (1 + tan2 B) − tan2 B (1+ tan2 A)
= tan2 A + tan2 A tan2 B − tan2 B − tan2 A tan2 B
= tan2A − tan2B
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. = x2 − y2
= (a sec θ + b tan θ)2 − (a tan θ + b sec θ)2
= a2 sec2 θ + b2 tan2 θ + 2ab sec θ tan θ − a2 tan2 θ − b2 sec2 θ – 2ab sec θ tan θ
= a2 sec2 θ + b2 tan2 θ − a2 tan2 θ − b2 sec2 θ
= a2 sec2 θ − b2 sec2 θ + b2 tan2θ − a2 tan2 θ
= sec2 θ (a2 − b2) + tan2 θ (b2 − a2)
= sec2θ (a2 − b2) − tan2θ (a2 − b2)
= (sec2 θ − tan2θ) (a2 − b2)
= a2 − b2
= R.H.S.
Hence proved.
Solution:
We are given,
=> 3 sin θ + 5 cos θ = 5
=> 3 sin θ = 5 (1 − cos θ)
=> 3 sin θ =
=> 3 sin θ =
=> 3 sin θ =
=> 3 (1 + cos θ) = 5 sin θ
=> 3 + 3 cos θ = 5 sin θ
=> 5 sin θ − 3 cos θ = 3
Hence proved.
Solution:
We have,
L.H.S. = m n
= (cosec θ + cot θ) (cosec θ – cot θ)
= cosec2 θ − cot2 θ
= 1
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
=
=
=
=
= sin2 θ cos2 θ
And R.H.S. =
=
=
=
=
= sin2 θ cos2 θ
Therefore, L.H.S. = R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
= (tan θ + sec θ)2 + (tan θ – sec θ)2
= tan2θ + sec2θ + 2 tan θ sec θ + tan2 θ + sec2θ – 2 tan θ sec θ
= 2[tan2 θ + sec2 θ]
= 2[]
= 2[]
= 2[]
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
=
=
=
=
=
=
=
=
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
=
=
=
=
=
=
=
=
=
=
=
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
=
=
=
= sec θ − tan θ
= 1/cos θ − sin θ/cos θ
=
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. = (sec A + tan A − 1) (sec A - tan A + 1)
= [sec A + tan A − (sec A + tan A) (sec A – tan A)] [sec A – tan A + (sec A – tan A)(sec A + tan A)]
= (sec A + tan A) (1 − (sec A – tan A)) (sec A – tan A) (1 + (sec A + tan A))
= (sec2 A − tan2 A) (1 – sec A + tan A) (1 + sec A + tan A)
= (1 – sec A + tan A) (1 + sec A + tan A)
= (1 – 1/cos A + sin A/cos A) (1 + 1/cos A + sin A/cos A)
=
=
=
=
= sin A/cos A
= 2 tan A
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. = (1 + cot A − cosec A)(1 + tan A + sec A)
= (1 + cos A/sin A − 1/sin A)(1 + sin A/cos A + 1/cos A)
=
=
=
=
= 2
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. = (cosec θ – sec θ) (cot θ – tan θ)
=
=
=
And R.H.S. = (cosec θ + sec θ) (sec θ cosec θ − 2)
=
=
=
=
=
Therefore, L.H.S. = R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
=
=
=
= cosec A − sec A
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
=
=
=
=
=
=
= 1
= R.H.S.
Hence proved.
Solution:
We have,
=
=
=
= sin A cos3 A + cos A sin3 A
= sin A cos A (sin2 A + cos2 A)
= sin A cos A
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. = sec4 A (1 − sin4 A) – 2 tan2 A
= sec4 A - tan4 A – 2 tan4 A
= (sec2 A)2 - tan4 A – 2 tan4 A
= (1+ tan2 A)2 − tan4 A − 2tan4 A
= 1 + tan4 A + 2tan2 A − tan4 A − 2tan4 A
= 1
= R.H.S.
Hence proved.
Solution:
We have,
L.H.S. =
=
=
=
And R.H.S. =
=
=
=
=
=
=
=
Therefore, L.H.S. = R.H.S.
Hence proved.
Solution:
We have,
L.H.S. = (1 + cot A + tan A) (sin A – cos A)
= sin A – cos A + cot A sin A – cot A cos A + sin A tan A – tan A cos A
= sin A – cos A + cos A – cot A cos A + sin A tan A – sin A
= sin A tan A – cos A cot A
= R.H.S
Hence proved.
Solution:
We have,
x cos θ/a + y sin θ/b = 1 . . . . (1)
x cos θ/a – y sin θ/b = 1 . . . . (2)
On squaring both sides of (1) and (2) and adding them we get,
=> (x cos θ/a + y sin θ/b)2 + (x cos θ/a – y sin θ/b)2 = 1 + 1
=> = 2
=> = 2
=> = 2
Hence proved.
Solution:
We are given,
=> cosec θ – sin θ = a3
=> 1/sin θ – sin θ = a3
=> a3 =
=> a3 =
=> a =
On squaring both sides, we get,
=> a2 =
Also we have,
=> sec θ – cos θ = b3
=> 1/cos θ – cos θ = b3
=> b3 =
=> b3 =
=> b =
On squaring both sides, we get,
=> b2 =
So, L.H.S. = a2b2 (a2+ b2)
=
=
= 1
= R.H.S.
Hence proved.
Solution:
We are given,
m = a cos3 θ + 3a cos θ sin2 θ and n = a sin3 θ + 3a cos2 θ sin θ
So, L.H.S. =
= (a cos3 θ + 3a cos θ sin2 θ + a sin3 θ + 3a cos2 θ sin θ)2/3 + (a cos3 θ + 3a cos θ sin2 θ – a sin3 θ – 3a cos2 θ sin θ)2/3
= a2/3 ((cos θ + sin θ)3)2/3 + a2/3 ((cos θ − sin θ)3)2/3
= a2/3 [(cos θ + sin θ)2 + (cos θ − sin θ)2]
= a2/3 [cos2 θ + sin2 θ + 2 sin θ cos θ + cos2 θ + sin2 θ − 2 sin θ cos θ]
= 2 a2/3
= R.H.S.
Hence proved.
Solution:
Given x = a cos3 θ and y = b sin3 θ.
So, L.H.S. = (x/a)2/3 + (y/b)2/3
=
= (cos3 θ)2/3 + (sin3 θ)2/3
= cos2 θ + sin2 θ
= 1
= R.H.S.
Hence proved.
Solution:
We have,
R.H.S = m2 + n2
= (a cos θ + b sin θ)2 + (a sin θ – b cos θ)2
= a2 cos2 θ + b2 sin2θ + 2ab sin θ cos θ + a2 sin2 θ + b2 cos2 θ – 2ab sin θ cos θ
= a2 cos2 θ + a2 cos2 θ + b2 sin2 θ + b2 cos2 θ
= a2 (sin2 θ + cos2 θ) + b2 (sin2 θ + cos2 θ)
= a2 + b2
= L.H.S.
Hence proved.
Solution:
We are given,
=> cos A + cos2 A = 1
=> cos A = 1 − cos2 A
=> cos A = sin2 A . . . . (1)
Now, L.H.S. = sin2 A + sin4 A
Using (1), we get,
= cos A + cos2 A
= 1
= R.H.S.
Hence proved.
Solution:
We are given,
=> cos θ + cos2 θ = 1
=> cos θ = 1 − cos2 θ
=> cos θ = sin2 θ . . . . (1)
Now, L.H.S. = sin12 θ + 3 sin10 θ + 3 sin8 θ + sin6 θ + 2 sin4 θ + 2 sin2 θ − 2
= (sin4 θ)3 + 3 sin4 θ sin2 θ (sin4 θ + sin2 θ) + (sin2 θ)3 + 2(sin2 θ)2 + 2 sin2 θ − 2
Using (1), we get,
= (sin4 θ + sin2 θ)3 + 2cos2 θ + 2 cos θ − 2
= ((sin2 θ)2 + sin2 θ)3 + 2 cos2 θ + 2 cos θ – 2
= (cos2 θ + sin2 θ)3 + 2 cos2 θ + 2 cos θ − 2
= 1 + 2(cos2 θ + sin2 θ) − 2
= 1 + 2(1) −2
= 1
= R.H.S.
Hence proved.
Solution:
We have,
= (1 + cos α)(1 + cos β)(1 + cos γ)
= 2 cos2 (α/2).2 cos2 (β/2).2 cos2 (γ/2)
=
=
=
Therefore, sin α sin β sin γ is the member of equality.
Hence proved.
Solution:
We are given,
=> sin θ + cos θ = x
On squaring both sides, we get,
=> (sin θ + cos θ)2 = x2
=> sin2 θ + cos2 θ + 2 sin θ cos θ = x2
=> 2 sin θ cos θ = x2 − 1
=> sin θ cos θ = (x2 − 1)/2 . . . . (1)
We know,
=> sin2 θ + cos2 θ = 1
Cubing on both sides, we get
=> (sin2 θ + cos2 θ)3 = 13
=> sin6 θ + cos6 θ + 3 sin2 θ cos2 θ (sin2 θ + cos2 θ) = 1
=> sin6 θ + cos6 θ = 1 – 3 sin2 θ cos2θ
From (1), we get,
=> sin6 θ + cos6 θ = 1 –
=> sin6 θ + cos6 θ =
Hence proved.
Solution:
We are given, x = a sec θ cos ϕ, y = b sec θ sin ϕ, z = c tan ϕ
On squaring x, y, z, we get,
x2 = a2 sec2 θ cos2 ϕ or x2/a2 = sec2 θ cos2 ϕ . . . . (1)
y2 = b2 sec2 θ sin2 ϕ or y2/b2 = sec2 θ sin2 ϕ . . . . (2)
z2 = c2 tan2 ϕ or z2/c2 = tan2 ϕ . . . . (3)
Now L.H.S. = x2/a2 + y2/b2 − z2/c2
Using (1), (2) and (3), we get,
= sec2 θ cos2 ϕ + sec2 θ sin2 ϕ − tan2 ϕ
= sec2θ (cos2 ϕ + sin2 ϕ) − tan2 ϕ
= sec2θ (1) − tan2 ϕ
= sec2 θ − tan2 θ
= 1
= R.H.S.
Hence proved.
Solution:
We are given, sin θ + 2 cos θ = 1
On squaring both sides, we get,
=> (sin θ + 2 cos θ)2 = 12
=> sin2 θ + 4 cos2 θ + 4 sin θ cos θ = 1
=> 4 cos2 θ + 4 sin θ cos θ = 1 – sin2 θ
=> 4 cos2 θ + 4 sin θ cos θ – cos2 θ = 0
=> 3 cos2 θ + 4 sin θ cos θ = 0 . . . . (1)
We have, L.H.S. = 2 sin θ – cos θ
On squaring L.H.S., we get,
= (2 sin θ – cos θ)2
= 4 sin2 θ + cos2 θ – 4 sin θ cos θ
From (1), we get,
= 4 sin2 θ + cos2 θ + 3 cos2θ
= 4 sin2 θ + 4 cos2 θ
= 4(sin2 θ + cos2 θ)
= 4
So, we have,
=> (2 sin θ – cos θ)2 = 4
=> 2 sin θ – cos θ = 2
Hence proved.