To determine the collinearity of the three points P , Q , P, Q, P , Q , and R R R , we analyze their coordinates using vector algebra and determinant properties.
Let the given points be represented as:
P = ( x 1 , y 1 ) = ( − sin ( β − α ) , − cos β ) P = (x_1, y_1) = (-\sin(\beta-\alpha), -\cos \beta) P = ( x 1 , y 1 ) = ( − sin ( β − α ) , − cos β )
Q = ( x 2 , y 2 ) = ( cos ( β − α ) , sin β ) Q = (x_2, y_2) = (\cos(\beta-\alpha), \sin \beta) Q = ( x 2 , y 2 ) = ( cos ( β − α ) , sin β )
R = ( x 3 , y 3 ) = ( cos ( β − α + θ ) , sin ( β − θ ) ) R = (x_3, y_3) = (\cos(\beta-\alpha+\theta), \sin(\beta-\theta)) R = ( x 3 , y 3 ) = ( cos ( β − α + θ ) , sin ( β − θ ))
Step 1: Express R R R in terms of P P P and Q Q Q
Using the trigonometric angle sum and difference formulas for x 3 x_3 x 3 and y 3 y_3 y 3 :
For x 3 x_3 x 3 :
x 3 = cos ( β − α + θ ) = cos ( β − α ) cos θ − sin ( β − α ) sin θ x_3 = \cos(\beta-\alpha+\theta) = \cos(\beta-\alpha)\cos\theta - \sin(\beta-\alpha)\sin\theta x 3 = cos ( β − α + θ ) = cos ( β − α ) cos θ − sin ( β − α ) sin θ
Substituting x 2 = cos ( β − α ) x_2 = \cos(\beta-\alpha) x 2 = cos ( β − α ) and x 1 = − sin ( β − α ) x_1 = -\sin(\beta-\alpha) x 1 = − sin ( β − α ) :
x 3 = x 2 cos θ + x 1 sin θ x_3 = x_2 \cos\theta + x_1 \sin\theta x 3 = x 2 cos θ + x 1 sin θ
For y 3 y_3 y 3 :
y 3 = sin ( β − θ ) = sin β cos θ − cos β sin θ y_3 = \sin(\beta-\theta) = \sin\beta\cos\theta - \cos\beta\sin\theta y 3 = sin ( β − θ ) = sin β cos θ − cos β sin θ
Substituting y 2 = sin β y_2 = \sin\beta y 2 = sin β and y 1 = − cos β y_1 = -\cos\beta y 1 = − cos β :
y 3 = y 2 cos θ + y 1 sin θ y_3 = y_2 \cos\theta + y_1 \sin\theta y 3 = y 2 cos θ + y 1 sin θ
Step 2: Formulate the Collinearity Determinant
Three points ( x 1 , y 1 ) (x_1, y_1) ( x 1 , y 1 ) , ( x 2 , y 2 ) (x_2, y_2) ( x 2 , y 2 ) , and ( x 3 , y 3 ) (x_3, y_3) ( x 3 , y 3 ) are collinear if and only if the determinant Δ \Delta Δ formed by their coordinates is zero:
Δ = ∣ x 1 y 1 1 x 2 y 2 1 x 3 y 3 1 ∣ \Delta = \begin{vmatrix} x_1 & y_1 & 1 \\ x_2 & y_2 & 1 \\ x_3 & y_3 & 1 \end{vmatrix} Δ = x 1 x 2 x 3 y 1 y 2 y 3 1 1 1
Substitute the relations x 3 = x 1 sin θ + x 2 cos θ x_3 = x_1 \sin\theta + x_2 \cos\theta x 3 = x 1 sin θ + x 2 cos θ and y 3 = y 1 sin θ + y 2 cos θ y_3 = y_1 \sin\theta + y_2 \cos\theta y 3 = y 1 sin θ + y 2 cos θ into the third row:
Δ = ∣ x 1 y 1 1 x 2 y 2 1 x 1 sin θ + x 2 cos θ y 1 sin θ + y 2 cos θ 1 ∣ \Delta = \begin{vmatrix} x_1 & y_1 & 1 \\ x_2 & y_2 & 1 \\ x_1 \sin\theta + x_2 \cos\theta & y_1 \sin\theta + y_2 \cos\theta & 1 \end{vmatrix} Δ = x 1 x 2 x 1 sin θ + x 2 cos θ y 1 y 2 y 1 sin θ + y 2 cos θ 1 1 1
Apply the row operation R 3 → R 3 − ( sin θ ) R 1 − ( cos θ ) R 2 R_3 \to R_3 - (\sin\theta) R_1 - (\cos\theta) R_2 R 3 → R 3 − ( sin θ ) R 1 − ( cos θ ) R 2 :
Δ = ∣ x 1 y 1 1 x 2 y 2 1 0 0 1 − sin θ − cos θ ∣ \Delta = \begin{vmatrix} x_1 & y_1 & 1 \\ x_2 & y_2 & 1 \\ 0 & 0 & 1 - \sin\theta - \cos\theta \end{vmatrix} Δ = x 1 x 2 0 y 1 y 2 0 1 1 1 − sin θ − cos θ
Expanding along the third row yields:
Δ = ( 1 − sin θ − cos θ ) ( x 1 y 2 − x 2 y 1 ) \Delta = (1 - \sin\theta - \cos\theta)(x_1 y_2 - x_2 y_1) Δ = ( 1 − sin θ − cos θ ) ( x 1 y 2 − x 2 y 1 )
Step 3: Evaluate x 1 y 2 − x 2 y 1 x_1 y_2 - x_2 y_1 x 1 y 2 − x 2 y 1
Using the definitions of x 1 , y 1 , x 2 , y 2 x_1, y_1, x_2, y_2 x 1 , y 1 , x 2 , y 2 :
x 1 y 2 − x 2 y 1 = ( − sin ( β − α ) ) ( sin β ) − ( cos ( β − α ) ) ( − cos β ) x_1 y_2 - x_2 y_1 = (-\sin(\beta-\alpha))(\sin\beta) - (\cos(\beta-\alpha))(-\cos\beta) x 1 y 2 − x 2 y 1 = ( − sin ( β − α )) ( sin β ) − ( cos ( β − α )) ( − cos β )
= cos ( β − α ) cos β − sin ( β − α ) sin β = \cos(\beta-\alpha)\cos\beta - \sin(\beta-\alpha)\sin\beta = cos ( β − α ) cos β − sin ( β − α ) sin β
Applying the cosine addition identity cos ( A + B ) = cos A cos B − sin A sin B \cos(A+B) = \cos A \cos B - \sin A \sin B cos ( A + B ) = cos A cos B − sin A sin B :
x 1 y 2 − x 2 y 1 = cos ( ( β − α ) + β ) = cos ( 2 β − α ) x_1 y_2 - x_2 y_1 = \cos((\beta-\alpha) + \beta) = \cos(2\beta - \alpha) x 1 y 2 − x 2 y 1 = cos (( β − α ) + β ) = cos ( 2 β − α )
Thus, the determinant simplifies to:
Δ = ( 1 − sin θ − cos θ ) cos ( 2 β − α ) \Delta = (1 - \sin\theta - \cos\theta)\cos(2\beta - \alpha) Δ = ( 1 − sin θ − cos θ ) cos ( 2 β − α )
Step 4: Check if Δ = 0 \Delta = 0 Δ = 0
Given the range 0 < α , β , θ < π 4 0 < \alpha, \beta, \theta < \frac{\pi}{4} 0 < α , β , θ < 4 π :
For the factor ( 1 − sin θ − cos θ ) (1 - \sin\theta - \cos\theta) ( 1 − sin θ − cos θ ) :
sin θ + cos θ = 2 sin ( θ + π 4 ) \sin\theta + \cos\theta = \sqrt{2}\sin\left(\theta + \frac{\pi}{4}\right) sin θ + cos θ = 2 sin ( θ + 4 π )
Since 0 < θ < π 4 0 < \theta < \frac{\pi}{4} 0 < θ < 4 π , we have π 4 < θ + π 4 < π 2 \frac{\pi}{4} < \theta + \frac{\pi}{4} < \frac{\pi}{2} 4 π < θ + 4 π < 2 π , which gives:
1 < sin θ + cos θ < 2 1 < \sin\theta + \cos\theta < \sqrt{2} 1 < sin θ + cos θ < 2
Therefore, ( 1 − sin θ − cos θ ) ≠ 0 (1 - \sin\theta - \cos\theta) \neq 0 ( 1 − sin θ − cos θ ) = 0 .
For the factor cos ( 2 β − α ) \cos(2\beta - \alpha) cos ( 2 β − α ) :
Since 0 < α < π 4 0 < \alpha < \frac{\pi}{4} 0 < α < 4 π and 0 < β < π 4 0 < \beta < \frac{\pi}{4} 0 < β < 4 π :
0 < 2 β < π 2 ⟹ − π 4 < 2 β − α < π 2 0 < 2\beta < \frac{\pi}{2} \implies -\frac{\pi}{4} < 2\beta - \alpha < \frac{\pi}{2} 0 < 2 β < 2 π ⟹ − 4 π < 2 β − α < 2 π
In the interval ( − π 4 , π 2 ) \left(-\frac{\pi}{4}, \frac{\pi}{2}\right) ( − 4 π , 2 π ) , the cosine function is strictly positive, so cos ( 2 β − α ) > 0 \cos(2\beta - \alpha) > 0 cos ( 2 β − α ) > 0 .
Since neither factor is zero, Δ ≠ 0 \Delta \neq 0 Δ = 0 .
Conclusion
Because the determinant is non-zero, the area of △ P Q R \triangle PQR △ P QR is non-zero, which means that the points P , Q , R P, Q, R P , Q , R are non-collinear .
Correct Answer: (D) P , Q , R P, Q, R P , Q , R are non-collinear