To match the expressions in Column I with their correct corresponding values in Column II , we evaluate each part step-by-step:
Part (A)
In Δ X Y Z \Delta XYZ Δ X Y Z , using the Sine Rule, the side lengths a , b , c a, b, c a , b , c opposite to angles X , Y , Z X, Y, Z X , Y , Z are given by:
a = 2 R sin X , b = 2 R sin Y , c = 2 R sin Z a = 2R \sin X, \quad b = 2R \sin Y, \quad c = 2R \sin Z a = 2 R sin X , b = 2 R sin Y , c = 2 R sin Z
Given the relation:
2 ( a 2 − b 2 ) = c 2 2(a^2 - b^2) = c^2 2 ( a 2 − b 2 ) = c 2
Substituting the sine expressions:
2 ( sin 2 X − sin 2 Y ) = sin 2 Z 2\left(\sin^2 X - \sin^2 Y\right) = \sin^2 Z 2 ( sin 2 X − sin 2 Y ) = sin 2 Z
Using the trigonometric identity sin 2 X − sin 2 Y = sin ( X − Y ) sin ( X + Y ) \sin^2 X - \sin^2 Y = \sin(X - Y)\sin(X + Y) sin 2 X − sin 2 Y = sin ( X − Y ) sin ( X + Y ) and the property X + Y + Z = π ⟹ sin ( X + Y ) = sin Z X + Y + Z = \pi \implies \sin(X + Y) = \sin Z X + Y + Z = π ⟹ sin ( X + Y ) = sin Z :
2 sin ( X − Y ) sin Z = sin 2 Z 2 \sin(X - Y) \sin Z = \sin^2 Z 2 sin ( X − Y ) sin Z = sin 2 Z
Since sin Z ≠ 0 \sin Z \neq 0 sin Z = 0 for a non-degenerate triangle, we divide both sides by sin Z \sin Z sin Z :
2 sin ( X − Y ) = sin Z ⟹ λ = sin ( X − Y ) sin Z = 1 2 2 \sin(X - Y) = \sin Z \implies \lambda = \frac{\sin(X - Y)}{\sin Z} = \frac{1}{2} 2 sin ( X − Y ) = sin Z ⟹ λ = s i n Z s i n ( X − Y ) = 2 1
Now, we are given:
cos ( n π λ ) = 0 ⟹ cos ( n π 2 ) = 0 \cos(n \pi \lambda) = 0 \implies \cos\left(\frac{n\pi}{2}\right) = 0 cos ( nπ λ ) = 0 ⟹ cos ( 2 nπ ) = 0
For cos ( n π 2 ) = 0 \cos\left(\frac{n\pi}{2}\right) = 0 cos ( 2 nπ ) = 0 , n π 2 \frac{n\pi}{2} 2 nπ must be an odd multiple of π 2 \frac{\pi}{2} 2 π , which implies n n n must be an odd integer (n = 1 , 3 , 5 , … n = 1, 3, 5, \dots n = 1 , 3 , 5 , … ).
From Column II, the odd integers are 1 , 3 , 1, 3, 1 , 3 , and 5 5 5 .
Thus, (A) matches with (P), (R), and (S) .
Part (B)
Given the trigonometric identity for Δ X Y Z \Delta XYZ Δ X Y Z :
1 + cos 2 X − 2 cos 2 Y = 2 sin X sin Y 1 + \cos 2X - 2\cos 2Y = 2\sin X \sin Y 1 + cos 2 X − 2 cos 2 Y = 2 sin X sin Y
Rewriting using double-angle identities 1 + cos 2 X = 2 cos 2 X 1 + \cos 2X = 2\cos^2 X 1 + cos 2 X = 2 cos 2 X and cos 2 Y = 1 − 2 sin 2 Y \cos 2Y = 1 - 2\sin^2 Y cos 2 Y = 1 − 2 sin 2 Y :
2 cos 2 X − 2 ( 1 − 2 sin 2 Y ) = 2 sin X sin Y 2\cos^2 X - 2(1 - 2\sin^2 Y) = 2\sin X \sin Y 2 cos 2 X − 2 ( 1 − 2 sin 2 Y ) = 2 sin X sin Y
Dividing by 2 2 2 and using cos 2 X = 1 − sin 2 X \cos^2 X = 1 - \sin^2 X cos 2 X = 1 − sin 2 X :
( 1 − sin 2 X ) − 1 + 2 sin 2 Y = sin X sin Y (1 - \sin^2 X) - 1 + 2\sin^2 Y = \sin X \sin Y ( 1 − sin 2 X ) − 1 + 2 sin 2 Y = sin X sin Y
2 sin 2 Y − sin X sin Y − sin 2 X = 0 2\sin^2 Y - \sin X \sin Y - \sin^2 X = 0 2 sin 2 Y − sin X sin Y − sin 2 X = 0
Dividing the entire equation by sin 2 Y \sin^2 Y sin 2 Y (since sin Y ≠ 0 \sin Y \neq 0 sin Y = 0 ) and letting t = sin X sin Y = a b > 0 t = \frac{\sin X}{\sin Y} = \frac{a}{b} > 0 t = s i n Y s i n X = b a > 0 :
2 − t − t 2 = 0 ⟹ t 2 + t − 2 = 0 2 - t - t^2 = 0 \implies t^2 + t - 2 = 0 2 − t − t 2 = 0 ⟹ t 2 + t − 2 = 0
( t + 2 ) ( t − 1 ) = 0 (t + 2)(t - 1) = 0 ( t + 2 ) ( t − 1 ) = 0
Since t = a b > 0 t = \frac{a}{b} > 0 t = b a > 0 , we get:
a b = 1 \frac{a}{b} = 1 b a = 1
Thus, (B) matches with (P) .
Part (C)
The position vectors are:
O X → = 3 i ^ + j ^ , O Y → = i ^ + 3 j ^ , O Z → = β i ^ + ( 1 − β ) j ^ \overrightarrow{OX} = \sqrt{3}\hat{i} + \hat{j}, \quad \overrightarrow{OY} = \hat{i} + \sqrt{3}\hat{j}, \quad \overrightarrow{OZ} = \beta\hat{i} + (1 - \beta)\hat{j} O X = 3 i ^ + j ^ , O Y = i ^ + 3 j ^ , O Z = β i ^ + ( 1 − β ) j ^
The magnitudes of O X → \overrightarrow{OX} O X and O Y → \overrightarrow{OY} O Y are both equal to 2 2 2 .
The unit vectors along O X → \overrightarrow{OX} O X and O Y → \overrightarrow{OY} O Y are:
u ^ X = 3 i ^ + j ^ 2 , u ^ Y = i ^ + 3 j ^ 2 \hat{u}_X = \frac{\sqrt{3}\hat{i} + \hat{j}}{2}, \quad \hat{u}_Y = \frac{\hat{i} + \sqrt{3}\hat{j}}{2} u ^ X = 2 3 i ^ + j ^ , u ^ Y = 2 i ^ + 3 j ^
The vector along the acute angle bisector is:
u ^ X + u ^ Y = 3 + 1 2 ( i ^ + j ^ ) \hat{u}_X + \hat{u}_Y = \frac{\sqrt{3}+1}{2}(\hat{i} + \hat{j}) u ^ X + u ^ Y = 2 3 + 1 ( i ^ + j ^ )
Since this direction is along i ^ + j ^ \hat{i} + \hat{j} i ^ + j ^ and passes through the origin O ( 0 , 0 ) O(0,0) O ( 0 , 0 ) , the line representing the acute angle bisector is:
x − y = 0 x - y = 0 x − y = 0
The distance d d d of point Z ( β , 1 − β ) Z(\beta, 1-\beta) Z ( β , 1 − β ) from the line x − y = 0 x - y = 0 x − y = 0 is given as 3 2 \frac{3}{\sqrt{2}} 2 3 :
d = ∣ β − ( 1 − β ) ∣ 1 2 + ( − 1 ) 2 = ∣ 2 β − 1 ∣ 2 = 3 2 d = \frac{|\beta - (1 - \beta)|}{\sqrt{1^2 + (-1)^2}} = \frac{|2\beta - 1|}{\sqrt{2}} = \frac{3}{\sqrt{2}} d = 1 2 + ( − 1 ) 2 ∣ β − ( 1 − β ) ∣ = 2 ∣2 β − 1∣ = 2 3
This simplifies to:
∣ 2 β − 1 ∣ = 3 |2\beta - 1| = 3 ∣2 β − 1∣ = 3
Solving for β \beta β :
2 β − 1 = 3 ⟹ β = 2 ⟹ ∣ β ∣ = 2 2\beta - 1 = 3 \implies \beta = 2 \implies |\beta| = 2 2 β − 1 = 3 ⟹ β = 2 ⟹ ∣ β ∣ = 2
2 β − 1 = − 3 ⟹ β = − 1 ⟹ ∣ β ∣ = 1 2\beta - 1 = -3 \implies \beta = -1 \implies |\beta| = 1 2 β − 1 = − 3 ⟹ β = − 1 ⟹ ∣ β ∣ = 1
Thus, the possible values of ∣ β ∣ |\beta| ∣ β ∣ are 1 1 1 and 2 2 2 .
Thus, (C) matches with (P) and (Q) .
Part (D)
Let g ( x ) = ∣ α x − 1 ∣ + ∣ α x − 2 ∣ + α x g(x) = |\alpha x - 1| + |\alpha x - 2| + \alpha x g ( x ) = ∣ α x − 1∣ + ∣ α x − 2∣ + α x . We need to compute the area F ( α ) F(\alpha) F ( α ) bounded by x = 0 x = 0 x = 0 , x = 2 x = 2 x = 2 , y 2 = 4 x ⟹ y = 2 x y^2 = 4x \implies y = 2\sqrt{x} y 2 = 4 x ⟹ y = 2 x (for y ≥ 0 y \ge 0 y ≥ 0 ), and y = g ( x ) y = g(x) y = g ( x ) .
Case 1: When α = 0 \alpha = 0 α = 0
g ( x ) = ∣ − 1 ∣ + ∣ − 2 ∣ + 0 = 3 g(x) = |-1| + |-2| + 0 = 3 g ( x ) = ∣ − 1∣ + ∣ − 2∣ + 0 = 3
Since 3 ≥ 2 x 3 \ge 2\sqrt{x} 3 ≥ 2 x for x ∈ [ 0 , 2 ] x \in [0, 2] x ∈ [ 0 , 2 ] , the area F ( 0 ) F(0) F ( 0 ) is:
F ( 0 ) = ∫ 0 2 ( 3 − 2 x ) d x = [ 3 x − 4 3 x 3 / 2 ] 0 2 = 6 − 8 2 3 F(0) = \int_{0}^{2} (3 - 2\sqrt{x}) \, dx = \left[ 3x - \frac{4}{3}x^{3/2} \right]_{0}^{2} = 6 - \frac{8\sqrt{2}}{3} F ( 0 ) = ∫ 0 2 ( 3 − 2 x ) d x = [ 3 x − 3 4 x 3/2 ] 0 2 = 6 − 3 8 2
Therefore:
F ( 0 ) + 8 3 2 = 6 F(0) + \frac{8}{3}\sqrt{2} = 6 F ( 0 ) + 3 8 2 = 6
Case 2: When α = 1 \alpha = 1 α = 1
g ( x ) = ∣ x − 1 ∣ + ∣ x − 2 ∣ + x g(x) = |x - 1| + |x - 2| + x g ( x ) = ∣ x − 1∣ + ∣ x − 2∣ + x
Breaking the domain x ∈ [ 0 , 2 ] x \in [0, 2] x ∈ [ 0 , 2 ] :
For x ∈ [ 0 , 1 ] x \in [0, 1] x ∈ [ 0 , 1 ] : g ( x ) = ( 1 − x ) + ( 2 − x ) + x = 3 − x g(x) = (1 - x) + (2 - x) + x = 3 - x g ( x ) = ( 1 − x ) + ( 2 − x ) + x = 3 − x
For x ∈ [ 1 , 2 ] x \in [1, 2] x ∈ [ 1 , 2 ] : g ( x ) = ( x − 1 ) + ( 2 − x ) + x = x + 1 g(x) = (x - 1) + (2 - x) + x = x + 1 g ( x ) = ( x − 1 ) + ( 2 − x ) + x = x + 1
For all x ∈ [ 0 , 2 ] x \in [0, 2] x ∈ [ 0 , 2 ] , g ( x ) ≥ 2 x g(x) \ge 2\sqrt{x} g ( x ) ≥ 2 x . The area F ( 1 ) F(1) F ( 1 ) is:
F ( 1 ) = ∫ 0 2 g ( x ) d x − ∫ 0 2 2 x d x F(1) = \int_{0}^{2} g(x) \, dx - \int_{0}^{2} 2\sqrt{x} \, dx F ( 1 ) = ∫ 0 2 g ( x ) d x − ∫ 0 2 2 x d x
Calculating ∫ 0 2 g ( x ) d x \int_{0}^{2} g(x) \, dx ∫ 0 2 g ( x ) d x :
∫ 0 1 ( 3 − x ) d x + ∫ 1 2 ( x + 1 ) d x = [ 3 x − x 2 2 ] 0 1 + [ x 2 2 + x ] 1 2 = 5 2 + 5 2 = 5 \int_{0}^{1} (3 - x) \, dx + \int_{1}^{2} (x + 1) \, dx = \left[ 3x - \frac{x^2}{2} \right]_{0}^{1} + \left[ \frac{x^2}{2} + x \right]_{1}^{2} = \frac{5}{2} + \frac{5}{2} = 5 ∫ 0 1 ( 3 − x ) d x + ∫ 1 2 ( x + 1 ) d x = [ 3 x − 2 x 2 ] 0 1 + [ 2 x 2 + x ] 1 2 = 2 5 + 2 5 = 5
Thus:
F ( 1 ) = 5 − 8 2 3 ⟹ F ( 1 ) + 8 3 2 = 5 F(1) = 5 - \frac{8\sqrt{2}}{3} \implies F(1) + \frac{8}{3}\sqrt{2} = 5 F ( 1 ) = 5 − 3 8 2 ⟹ F ( 1 ) + 3 8 2 = 5
Hence, the possible values of F ( α ) + 8 3 2 F(\alpha) + \frac{8}{3}\sqrt{2} F ( α ) + 3 8 2 are 5 5 5 and 6 6 6 .
Thus, (D) matches with (S) and (T) .
Final Match:
(A) → \rightarrow → (P), (R), (S)
(B) → \rightarrow → (P)
(C) → \rightarrow → (P), (Q)
(D) → \rightarrow → (S), (T)