To match the statements in Column I with the correct values in Column II , we analyze each part step-by-step:
(A)
We are given the vectors:
a ⃗ = j ^ + 3 k ^ , b ⃗ = − j ^ + 3 k ^ , c ⃗ = 2 3 k ^ \vec{a} = \hat{j} + \sqrt{3}\,\hat{k}, \quad \vec{b} = -\hat{j} + \sqrt{3}\,\hat{k}, \quad \vec{c} = 2\sqrt{3}\,\hat{k} a = j ^ + 3 k ^ , b = − j ^ + 3 k ^ , c = 2 3 k ^
Notice that:
a ⃗ + b ⃗ = ( j ^ + 3 k ^ ) + ( − j ^ + 3 k ^ ) = 2 3 k ^ = c ⃗ \vec{a} + \vec{b} = (\hat{j} + \sqrt{3}\,\hat{k}) + (-\hat{j} + \sqrt{3}\,\hat{k}) = 2\sqrt{3}\,\hat{k} = \vec{c} a + b = ( j ^ + 3 k ^ ) + ( − j ^ + 3 k ^ ) = 2 3 k ^ = c
Let the vertices of the triangle be A , B , A, B, A , B , and C C C such that:
A B ⃗ = a ⃗ , B C ⃗ = b ⃗ , and A C ⃗ = a ⃗ + b ⃗ = c ⃗ \vec{AB} = \vec{a}, \quad \vec{BC} = \vec{b}, \quad \text{and} \quad \vec{AC} = \vec{a} + \vec{b} = \vec{c} A B = a , B C = b , and A C = a + b = c
The two sides of the triangle meeting at vertex B B B are along the vectors B A ⃗ = − a ⃗ \vec{BA} = -\vec{a} B A = − a and B C ⃗ = b ⃗ \vec{BC} = \vec{b} B C = b .
The internal angle θ \theta θ between sides a ⃗ \vec{a} a and b ⃗ \vec{b} b at vertex B B B is given by:
cos θ = B A ⃗ ⋅ B C ⃗ ∣ B A ⃗ ∣ ∣ B C ⃗ ∣ = ( − a ⃗ ) ⋅ b ⃗ ∣ a ⃗ ∣ ∣ b ⃗ ∣ \cos\theta = \frac{\vec{BA} \cdot \vec{BC}}{|\vec{BA}||\vec{BC}|} = \frac{(-\vec{a}) \cdot \vec{b}}{|\vec{a}||\vec{b}|} cos θ = ∣ B A ∣∣ B C ∣ B A ⋅ B C = ∣ a ∣∣ b ∣ ( − a ) ⋅ b
First, compute the magnitudes and the dot product:
∣ a ⃗ ∣ = 0 2 + 1 2 + ( 3 ) 2 = 4 = 2 |\vec{a}| = \sqrt{0^2 + 1^2 + (\sqrt{3})^2} = \sqrt{4} = 2 ∣ a ∣ = 0 2 + 1 2 + ( 3 ) 2 = 4 = 2
∣ b ⃗ ∣ = 0 2 + ( − 1 ) 2 + ( 3 ) 2 = 4 = 2 |\vec{b}| = \sqrt{0^2 + (-1)^2 + (\sqrt{3})^2} = \sqrt{4} = 2 ∣ b ∣ = 0 2 + ( − 1 ) 2 + ( 3 ) 2 = 4 = 2
a ⃗ ⋅ b ⃗ = ( 0 ) ( 0 ) + ( 1 ) ( − 1 ) + ( 3 ) ( 3 ) = − 1 + 3 = 2 \vec{a} \cdot \vec{b} = (0)(0) + (1)(-1) + (\sqrt{3})(\sqrt{3}) = -1 + 3 = 2 a ⋅ b = ( 0 ) ( 0 ) + ( 1 ) ( − 1 ) + ( 3 ) ( 3 ) = − 1 + 3 = 2
Thus:
cos θ = − a ⃗ ⋅ b ⃗ ∣ a ⃗ ∣ ∣ b ⃗ ∣ = − 2 2 × 2 = − 1 2 \cos\theta = -\frac{\vec{a} \cdot \vec{b}}{|\vec{a}||\vec{b}|} = -\frac{2}{2 \times 2} = -\frac{1}{2} cos θ = − ∣ a ∣∣ b ∣ a ⋅ b = − 2 × 2 2 = − 2 1
Since θ ∈ ( 0 , π ) \theta \in (0, \pi) θ ∈ ( 0 , π ) , we have:
θ = 2 π 3 \theta = \frac{2\pi}{3} θ = 3 2 π
Therefore, (A) matches with (q) .
(B)
We are given:
∫ a b ( f ( x ) − 3 x ) d x = a 2 − b 2 \int_{a}^{b} (f(x) - 3x)\,dx = a^2 - b^2 ∫ a b ( f ( x ) − 3 x ) d x = a 2 − b 2
Rewriting the right-hand side in integral form:
a 2 − b 2 = − ( b 2 − a 2 ) = − ∫ a b 2 x d x a^2 - b^2 = -(b^2 - a^2) = -\int_{a}^{b} 2x\,dx a 2 − b 2 = − ( b 2 − a 2 ) = − ∫ a b 2 x d x
Thus:
∫ a b ( f ( x ) − 3 x ) d x = ∫ a b ( − 2 x ) d x \int_{a}^{b} (f(x) - 3x)\,dx = \int_{a}^{b} (-2x)\,dx ∫ a b ( f ( x ) − 3 x ) d x = ∫ a b ( − 2 x ) d x
∫ a b ( f ( x ) − x ) d x = 0 \int_{a}^{b} (f(x) - x)\,dx = 0 ∫ a b ( f ( x ) − x ) d x = 0
Assuming this relation holds identically for all real limits a a a and b b b , differentiating both sides with respect to b b b gives:
f ( b ) − b = 0 ⟹ f ( x ) = x f(b) - b = 0 \implies f(x) = x f ( b ) − b = 0 ⟹ f ( x ) = x
Evaluating at x = π 6 x = \frac{\pi}{6} x = 6 π :
f ( π 6 ) = π 6 f\left(\frac{\pi}{6}\right) = \frac{\pi}{6} f ( 6 π ) = 6 π
(Note: If the relation is only given for specific constants a a a and b b b , f ( π 6 ) f\left(\frac{\pi}{6}\right) f ( 6 π ) is not uniquely determined, leading to any value being possible. Hence, officially (p) or all options (p, q, r, s, t) are accepted).
Therefore, (B) matches with (p) [or (p, q, r, s, t) ].
(C)
We evaluate the integral:
I = ∫ − 1 / 6 1 / 6 sec ( π x ) d x I = \int_{-1/6}^{1/6} \sec(\pi x)\,dx I = ∫ − 1/6 1/6 sec ( π x ) d x
Using the substitution u = π x u = \pi x u = π x , so d u = π d x du = \pi\,dx d u = π d x :
I = 1 π ∫ − π / 6 π / 6 sec u d u I = \frac{1}{\pi}\int_{-\pi/6}^{\pi/6} \sec u\,du I = π 1 ∫ − π /6 π /6 sec u d u
Since sec u \sec u sec u is an even function:
I = 2 π ∫ 0 π / 6 sec u d u = 2 π [ ln ∣ sec u + tan u ∣ ] 0 π / 6 I = \frac{2}{\pi}\int_{0}^{\pi/6} \sec u\,du = \frac{2}{\pi}\left[ \ln|\sec u + \tan u| \right]_{0}^{\pi/6} I = π 2 ∫ 0 π /6 sec u d u = π 2 [ ln ∣ sec u + tan u ∣ ] 0 π /6
Evaluating at the limits:
sec ( π 6 ) = 2 3 , tan ( π 6 ) = 1 3 \sec\left(\frac{\pi}{6}\right) = \frac{2}{\sqrt{3}}, \quad \tan\left(\frac{\pi}{6}\right) = \frac{1}{\sqrt{3}} sec ( 6 π ) = 3 2 , tan ( 6 π ) = 3 1
sec ( π 6 ) + tan ( π 6 ) = 3 3 = 3 \sec\left(\frac{\pi}{6}\right) + \tan\left(\frac{\pi}{6}\right) = \frac{3}{\sqrt{3}} = \sqrt{3} sec ( 6 π ) + tan ( 6 π ) = 3 3 = 3
sec ( 0 ) + tan ( 0 ) = 1 \sec(0) + \tan(0) = 1 sec ( 0 ) + tan ( 0 ) = 1
Thus:
I = 2 π ln ( 3 ) = 2 π ( 1 2 ln 3 ) = ln 3 π I = \frac{2}{\pi}\ln(\sqrt{3}) = \frac{2}{\pi}\left(\frac{1}{2}\ln 3\right) = \frac{\ln 3}{\pi} I = π 2 ln ( 3 ) = π 2 ( 2 1 ln 3 ) = π l n 3
Now, substituting I I I into the given expression:
π 2 ln 3 ∫ − 1 / 6 1 / 6 sec ( π x ) d x = π 2 ln 3 × ln 3 π = π \frac{\pi^2}{\ln 3}\int_{-1/6}^{1/6} \sec(\pi x)\,dx = \frac{\pi^2}{\ln 3} \times \frac{\ln 3}{\pi} = \pi l n 3 π 2 ∫ − 1/6 1/6 sec ( π x ) d x = l n 3 π 2 × π l n 3 = π
Therefore, (C) matches with (s) .
(D)
We are given ∣ z ∣ = 1 |z| = 1 ∣ z ∣ = 1 with z ≠ 1 z \neq 1 z = 1 . Let z = e i θ z = e^{i\theta} z = e i θ where θ ∈ ( 0 , 2 π ) \theta \in (0, 2\pi) θ ∈ ( 0 , 2 π ) .
Then:
1 − z = 1 − e i θ = 1 − cos θ − i sin θ = 2 sin 2 ( θ 2 ) − 2 i sin ( θ 2 ) cos ( θ 2 ) 1 - z = 1 - e^{i\theta} = 1 - \cos\theta - i\sin\theta = 2\sin^2\left(\frac{\theta}{2}\right) - 2i\sin\left(\frac{\theta}{2}\right)\cos\left(\frac{\theta}{2}\right) 1 − z = 1 − e i θ = 1 − cos θ − i sin θ = 2 sin 2 ( 2 θ ) − 2 i sin ( 2 θ ) cos ( 2 θ )
1 − z = − 2 i sin ( θ 2 ) ( cos θ 2 + i sin θ 2 ) = 2 sin ( θ 2 ) e − i π / 2 e i θ / 2 = 2 sin ( θ 2 ) e i ( θ − π 2 ) 1 - z = -2i\sin\left(\frac{\theta}{2}\right)\left(\cos\frac{\theta}{2} + i\sin\frac{\theta}{2}\right) = 2\sin\left(\frac{\theta}{2}\right)e^{-i\pi/2}e^{i\theta/2} = 2\sin\left(\frac{\theta}{2}\right)e^{i\left(\frac{\theta - \pi}{2}\right)} 1 − z = − 2 i sin ( 2 θ ) ( cos 2 θ + i sin 2 θ ) = 2 sin ( 2 θ ) e − iπ /2 e i θ /2 = 2 sin ( 2 θ ) e i ( 2 θ − π )
Taking the reciprocal:
1 1 − z = 1 2 sin ( θ 2 ) e i ( π − θ 2 ) \frac{1}{1-z} = \frac{1}{2\sin\left(\frac{\theta}{2}\right)} e^{i\left(\frac{\pi - \theta}{2}\right)} 1 − z 1 = 2 s i n ( 2 θ ) 1 e i ( 2 π − θ )
Since θ ∈ ( 0 , 2 π ) \theta \in (0, 2\pi) θ ∈ ( 0 , 2 π ) , we have θ 2 ∈ ( 0 , π ) \frac{\theta}{2} \in (0, \pi) 2 θ ∈ ( 0 , π ) , which implies sin ( θ 2 ) > 0 \sin\left(\frac{\theta}{2}\right) > 0 sin ( 2 θ ) > 0 . Thus:
Arg ( 1 1 − z ) = π − θ 2 \operatorname{Arg}\left(\frac{1}{1-z}\right) = \frac{\pi - \theta}{2} Arg ( 1 − z 1 ) = 2 π − θ
As θ → 0 + \theta \to 0^+ θ → 0 + , Arg ( 1 1 − z ) → π 2 \operatorname{Arg}\left(\frac{1}{1-z}\right) \to \frac{\pi}{2} Arg ( 1 − z 1 ) → 2 π .
As θ → 2 π − \theta \to 2\pi^- θ → 2 π − , Arg ( 1 1 − z ) → − π 2 \operatorname{Arg}\left(\frac{1}{1-z}\right) \to -\frac{\pi}{2} Arg ( 1 − z 1 ) → − 2 π .
Hence:
∣ Arg ( 1 1 − z ) ∣ < π 2 \left|\operatorname{Arg}\left(\frac{1}{1-z}\right)\right| < \frac{\pi}{2} Arg ( 1 − z 1 ) < 2 π
The maximum (supremum) value attained is:
π 2 \frac{\pi}{2} 2 π
Therefore, (D) matches with (t) .
Final Matching:
A → \to → q
B → \to → p (or p, q, r, s, t )
C → \to → s
D → \to → t