JEE Challenger
More from Three Dimensional Geometry

Match Column Statements for Lines Vectors Functions and Integrals

Match the statements in Column-I with the values in Column-II.

Column IColumn IIA) A line from the origin meets the lines x−21=y−1−2=z+11 and x−832=y+3−1=z−11 at P and Qp) −4respectively. If length PQ=d, then d2 isB) The values of x satisfying tan⁡−1(x+3)−tan⁡−1(x−3)=sin⁡−1(35) areq) 0C) Non-zero vectors a⃗,b⃗ and c⃗ satisfy a⃗⋅b⃗=0,(b⃗−a⃗)⋅(b⃗+c⃗)=0 and 2∣b⃗+c⃗∣=∣b⃗−a⃗∣.r) 4If a⃗=μb⃗+4c⃗, then the possible values of μ areD) Let f be the function on [−π,π] given by f(0)=9 and f(x)=sin⁡(9x2)/sin⁡(x2) for x≠0.s) 5The value of 2π∫−ππf(x) dx ist) 6\begin{array}{l l} \text{\textbf{Column I}} & \text{\textbf{Column II}} \\ \text{A) A line from the origin meets the lines } \frac{x-2}{1} = \frac{y-1}{-2} = \frac{z+1}{1} \text{ and } \frac{x-\frac{8}{3}}{2} = \frac{y+3}{-1} = \frac{z-1}{1} \text{ at } P \text{ and } Q & \text{p) } -4 \\ \quad \text{respectively. If length } PQ = d\text{, then } d^2 \text{ is} & \\ \text{B) The values of } x \text{ satisfying } \tan^{-1}(x+3) - \tan^{-1}(x-3) = \sin^{-1}\left(\frac{3}{5}\right) \text{ are} & \text{q) } 0 \\ \text{C) Non-zero vectors } \vec{a}, \vec{b} \text{ and } \vec{c} \text{ satisfy } \vec{a} \cdot \vec{b} = 0, (\vec{b}-\vec{a}) \cdot (\vec{b}+\vec{c}) = 0 \text{ and } 2|\vec{b}+\vec{c}| = |\vec{b}-\vec{a}|. & \text{r) } 4 \\ \quad \text{If } \vec{a} = \mu\vec{b} + 4\vec{c}\text{, then the possible values of } \mu \text{ are} & \\ \text{D) Let } f \text{ be the function on } [-\pi, \pi] \text{ given by } f(0) = 9 \text{ and } f(x) = \sin\left(\frac{9x}{2}\right) \Big/ \sin\left(\frac{x}{2}\right) \text{ for } x \neq 0. & \text{s) } 5 \\ \quad \text{The value of } \frac{2}{\pi}\int_{-\pi}^{\pi} f(x)\,dx \text{ is} & \text{t) } 6 \end{array}

Options

A

(A)→(T),  (B)→(P),  (C)→(Q,S),  (D)→(R)(\text{A}) \rightarrow (\text{T}),\; (\text{B}) \rightarrow (\text{P}),\; (\text{C}) \rightarrow (\text{Q}, \text{S}),\; (\text{D}) \rightarrow (\text{R})

B

(A)→(T),  (B)→(P,R),  (C)→(Q,S),  (D)→(R)(\text{A}) \rightarrow (\text{T}),\; (\text{B}) \rightarrow (\text{P}, \text{R}),\; (\text{C}) \rightarrow (\text{Q}, \text{S}),\; (\text{D}) \rightarrow (\text{R})

Correct
C

(A)→(T),  (B)→(P,R),  (C)→(Q),  (D)→(R)(\text{A}) \rightarrow (\text{T}),\; (\text{B}) \rightarrow (\text{P}, \text{R}),\; (\text{C}) \rightarrow (\text{Q}),\; (\text{D}) \rightarrow (\text{R})

D

(A)→(S,T),  (B)→(R),  (C)→(Q,S),  (D)→(P,R)(\text{A}) \rightarrow (\text{S}, \text{T}),\; (\text{B}) \rightarrow (\text{R}),\; (\text{C}) \rightarrow (\text{Q}, \text{S}),\; (\text{D}) \rightarrow (\text{P}, \text{R})

Step-by-Step Solution

To solve the given matching problem, we analyze each column statement step-by-step.


Part A

The given lines are:
L1:x−21=y−1−2=z+11=λL_1: \frac{x-2}{1} = \frac{y-1}{-2} = \frac{z+1}{1} = \lambda
L2:x−832=y+3−1=z−11=μL_2: \frac{x-\frac{8}{3}}{2} = \frac{y+3}{-1} = \frac{z-1}{1} = \mu

Any general point PP on L1L_1 and QQ on L2L_2 can be represented as:
P=(λ+2,−2λ+1,λ−1)P = (\lambda + 2, -2\lambda + 1, \lambda - 1)
Q=(2μ+83,−μ−3,μ+1)Q = \left(2\mu + \frac{8}{3}, -\mu - 3, \mu + 1\right)

Since PP, QQ, and the origin O(0,0,0)O(0,0,0) lie on the same line, the position vectors OP⃗\vec{OP} and OQ⃗\vec{OQ} are collinear. Thus, their corresponding coordinates must be proportional:
λ+22μ+83=−2λ+1−μ−3=λ−1μ+1\frac{\lambda + 2}{2\mu + \frac{8}{3}} = \frac{-2\lambda + 1}{-\mu - 3} = \frac{\lambda - 1}{\mu + 1}

Equating the second and third ratios:
2λ−1μ+3=λ−1μ+1\frac{2\lambda - 1}{\mu + 3} = \frac{\lambda - 1}{\mu + 1}
(2λ−1)(μ+1)=(λ−1)(μ+3)(2\lambda - 1)(\mu + 1) = (\lambda - 1)(\mu + 3)
2λμ+2λ−μ−1=λμ+3λ−μ−32\lambda\mu + 2\lambda - \mu - 1 = \lambda\mu + 3\lambda - \mu - 3
λμ−λ+2=0  ⟹  λμ=λ−2— (1)\lambda\mu - \lambda + 2 = 0 \implies \lambda\mu = \lambda - 2 \quad \text{--- (1)}

Equating the first and third ratios:
(λ+2)(μ+1)=(λ−1)(2μ+83)(\lambda + 2)(\mu + 1) = (\lambda - 1)\left(2\mu + \frac{8}{3}\right)
λμ+λ+2μ+2=2λμ+83λ−2μ−83\lambda\mu + \lambda + 2\mu + 2 = 2\lambda\mu + \frac{8}{3}\lambda - 2\mu - \frac{8}{3}
λμ+53λ−4μ−143=0— (2)\lambda\mu + \frac{5}{3}\lambda - 4\mu - \frac{14}{3} = 0 \quad \text{--- (2)}

Substituting λμ=λ−2\lambda\mu = \lambda - 2 into (2):
(λ−2)+53λ−4μ−143=0(\lambda - 2) + \frac{5}{3}\lambda - 4\mu - \frac{14}{3} = 0
83λ−4μ−203=0  ⟹  μ=2λ−53— (3)\frac{8}{3}\lambda - 4\mu - \frac{20}{3} = 0 \implies \mu = \frac{2\lambda - 5}{3} \quad \text{--- (3)}

Substitute (3) back into (1):
λ(2λ−53)=λ−2\lambda \left(\frac{2\lambda - 5}{3}\right) = \lambda - 2
2λ2−8λ+6=0  ⟹  λ2−4λ+3=0  ⟹  λ=1 or λ=32\lambda^2 - 8\lambda + 6 = 0 \implies \lambda^2 - 4\lambda + 3 = 0 \implies \lambda = 1 \text{ or } \lambda = 3

  • For λ=1\lambda = 1, μ=−1\mu = -1, the point P=(3,−1,0)P = (3, -1, 0) and Q=(23,−2,0)Q = \left(\frac{2}{3}, -2, 0\right) are not collinear with O(0,0,0)O(0,0,0) because 32/3≠−1−2\frac{3}{2/3} \neq \frac{-1}{-2}.
  • For λ=3\lambda = 3, μ=13\mu = \frac{1}{3}, the points are:
    P=(5,−5,2)P = (5, -5, 2)
    Q=(103,−103,43)=23PQ = \left(\frac{10}{3}, -\frac{10}{3}, \frac{4}{3}\right) = \frac{2}{3} P

Since Q=23PQ = \frac{2}{3}P, O,P,QO, P, Q are collinear.
The vector PQ⃗=OQ⃗−OP⃗=−13OP⃗\vec{PQ} = \vec{OQ} - \vec{OP} = -\frac{1}{3} \vec{OP}.
Hence, the distance dd is:
d2=∣PQ⃗∣2=19∣OP⃗∣2=19(52+(−5)2+22)=549=6d^2 = |\vec{PQ}|^2 = \frac{1}{9} |\vec{OP}|^2 = \frac{1}{9} (5^2 + (-5)^2 + 2^2) = \frac{54}{9} = 6

Matching for A: t


Part B

Given equation:
tan⁡−1(x+3)−tan⁡−1(x−3)=sin⁡−1(35)\tan^{-1}(x+3) - \tan^{-1}(x-3) = \sin^{-1}\left(\frac{3}{5}\right)

Taking tangent on both sides (using tan⁡(sin⁡−1(3/5))=34\tan(\sin^{-1}(3/5)) = \frac{3}{4}):
tan⁡(tan⁡−1(x+3)−tan⁡−1(x−3))=34\tan\left(\tan^{-1}(x+3) - \tan^{-1}(x-3)\right) = \frac{3}{4}
(x+3)−(x−3)1+(x+3)(x−3)=34\frac{(x+3) - (x-3)}{1 + (x+3)(x-3)} = \frac{3}{4}
61+x2−9=34  ⟹  6x2−8=34\frac{6}{1 + x^2 - 9} = \frac{3}{4} \implies \frac{6}{x^2 - 8} = \frac{3}{4}
3(x2−8)=24  ⟹  x2−8=8  ⟹  x2=16  ⟹  x=±43(x^2 - 8) = 24 \implies x^2 - 8 = 8 \implies x^2 = 16 \implies x = \pm 4

Checking both values:

  • For x=4x = 4: tan⁡−1(7)−tan⁡−1(1)=tan⁡−1(7−11+7)=tan⁡−1(34)=sin⁡−1(35)\tan^{-1}(7) - \tan^{-1}(1) = \tan^{-1}\left(\frac{7-1}{1+7}\right) = \tan^{-1}\left(\frac{3}{4}\right) = \sin^{-1}\left(\frac{3}{5}\right) (Valid).
  • For x=−4x = -4: tan⁡−1(−1)−tan⁡−1(−7)=tan⁡−1(7)−tan⁡−1(1)=sin⁡−1(35)\tan^{-1}(-1) - \tan^{-1}(-7) = \tan^{-1}(7) - \tan^{-1}(1) = \sin^{-1}\left(\frac{3}{5}\right) (Valid).

Matching for B: p, r


Part C

Given conditions:

  1. a⃗⋅b⃗=0\vec{a} \cdot \vec{b} = 0
  2. (b⃗−a⃗)⋅(b⃗+c⃗)=0  ⟹  ∣b⃗∣2+b⃗⋅c⃗−a⃗⋅c⃗=0(\vec{b}-\vec{a}) \cdot (\vec{b}+\vec{c}) = 0 \implies |\vec{b}|^2 + \vec{b}\cdot\vec{c} - \vec{a}\cdot\vec{c} = 0
  3. 2∣b⃗+c⃗∣=∣b⃗−a⃗∣  ⟹  4∣b⃗+c⃗∣2=∣b⃗−a⃗∣22|\vec{b}+\vec{c}| = |\vec{b}-\vec{a}| \implies 4|\vec{b}+\vec{c}|^2 = |\vec{b}-\vec{a}|^2
    4(∣b⃗∣2+∣c⃗∣2+2b⃗⋅c⃗)=∣b⃗∣2+∣a⃗∣24(|\vec{b}|^2 + |\vec{c}|^2 + 2\vec{b}\cdot\vec{c}) = |\vec{b}|^2 + |\vec{a}|^2
    3∣b⃗∣2+4∣c⃗∣2+8b⃗⋅c⃗=∣a⃗∣2— (1)3|\vec{b}|^2 + 4|\vec{c}|^2 + 8\vec{b}\cdot\vec{c} = |\vec{a}|^2 \quad \text{--- (1)}

Given a⃗=μb⃗+4c⃗\vec{a} = \mu\vec{b} + 4\vec{c}, take dot product with b⃗\vec{b}:
a⃗⋅b⃗=μ∣b⃗∣2+4b⃗⋅c⃗=0  ⟹  b⃗⋅c⃗=−μ4∣b⃗∣2\vec{a}\cdot\vec{b} = \mu|\vec{b}|^2 + 4\vec{b}\cdot\vec{c} = 0 \implies \vec{b}\cdot\vec{c} = -\frac{\mu}{4}|\vec{b}|^2

From condition (2):
a⃗⋅c⃗=∣b⃗∣2+b⃗⋅c⃗=∣b⃗∣2(1−μ4)\vec{a}\cdot\vec{c} = |\vec{b}|^2 + \vec{b}\cdot\vec{c} = |\vec{b}|^2 \left(1 - \frac{\mu}{4}\right)

Now, compute ∣a⃗∣2|\vec{a}|^2:
∣a⃗∣2=a⃗⋅(μb⃗+4c⃗)=4(a⃗⋅c⃗)=4∣b⃗∣2(1−μ4)=∣b⃗∣2(4−μ)|\vec{a}|^2 = \vec{a}\cdot(\mu\vec{b} + 4\vec{c}) = 4(\vec{a}\cdot\vec{c}) = 4|\vec{b}|^2 \left(1 - \frac{\mu}{4}\right) = |\vec{b}|^2 (4 - \mu)

Also, from a⃗=μb⃗+4c⃗\vec{a} = \mu\vec{b} + 4\vec{c}:
∣a⃗∣2=μ2∣b⃗∣2+16∣c⃗∣2+8μ(b⃗⋅c⃗)=μ2∣b⃗∣2+16∣c⃗∣2−2μ2∣b⃗∣2=16∣c⃗∣2−μ2∣b⃗∣2|\vec{a}|^2 = \mu^2|\vec{b}|^2 + 16|\vec{c}|^2 + 8\mu(\vec{b}\cdot\vec{c}) = \mu^2|\vec{b}|^2 + 16|\vec{c}|^2 - 2\mu^2|\vec{b}|^2 = 16|\vec{c}|^2 - \mu^2|\vec{b}|^2

Equating the two expressions for ∣a⃗∣2|\vec{a}|^2:
∣b⃗∣2(4−μ)=16∣c⃗∣2−μ2∣b⃗∣2  ⟹  16∣c⃗∣2=∣b⃗∣2(μ2−μ+4)|\vec{b}|^2(4 - \mu) = 16|\vec{c}|^2 - \mu^2|\vec{b}|^2 \implies 16|\vec{c}|^2 = |\vec{b}|^2(\mu^2 - \mu + 4)

Substitute ∣c⃗∣2|\vec{c}|^2, b⃗⋅c⃗\vec{b}\cdot\vec{c}, and ∣a⃗∣2|\vec{a}|^2 into (1):
3∣b⃗∣2+4(∣b⃗∣2(μ2−μ+4)16)+8(−μ4∣b⃗∣2)=∣b⃗∣2(4−μ)3|\vec{b}|^2 + 4\left(\frac{|\vec{b}|^2(\mu^2 - \mu + 4)}{16}\right) + 8\left(-\frac{\mu}{4}|\vec{b}|^2\right) = |\vec{b}|^2(4 - \mu)

Dividing by ∣b⃗∣2≠0|\vec{b}|^2 \neq 0:
3+μ2−μ+44−2μ=4−μ3 + \frac{\mu^2 - \mu + 4}{4} - 2\mu = 4 - \mu
12+μ2−μ+4−8μ=16−4μ12 + \mu^2 - \mu + 4 - 8\mu = 16 - 4\mu
μ2−5μ=0  ⟹  μ=0 or μ=5\mu^2 - 5\mu = 0 \implies \mu = 0 \text{ or } \mu = 5

Matching for C: q, s (or q)


Part D

Given function:
f(x)=sin⁡(9x2)sin⁡(x2)for x≠0, and f(0)=9f(x) = \frac{\sin\left(\frac{9x}{2}\right)}{\sin\left(\frac{x}{2}\right)} \quad \text{for } x \neq 0, \text{ and } f(0) = 9

Using the trigonometric identity:
sin⁡((2n+1)x2)sin⁡(x2)=1+2∑k=1ncos⁡(kx)\frac{\sin\left((2n+1)\frac{x}{2}\right)}{\sin\left(\frac{x}{2}\right)} = 1 + 2\sum_{k=1}^{n} \cos(kx)

For n=4n = 4:
f(x)=1+2cos⁡(x)+2cos⁡(2x)+2cos⁡(3x)+2cos⁡(4x)f(x) = 1 + 2\cos(x) + 2\cos(2x) + 2\cos(3x) + 2\cos(4x)

Since f(x)f(x) is an even function:
∫−ππf(x) dx=2∫0π(1+2cos⁡(x)+2cos⁡(2x)+2cos⁡(3x)+2cos⁡(4x)) dx\int_{-\pi}^{\pi} f(x) \, dx = 2 \int_{0}^{\pi} \left(1 + 2\cos(x) + 2\cos(2x) + 2\cos(3x) + 2\cos(4x)\right) \, dx
=2[x+2sin⁡(x)+sin⁡(2x)+23sin⁡(3x)+12sin⁡(4x)]0π=2π= 2 \left[ x + 2\sin(x) + \sin(2x) + \frac{2}{3}\sin(3x) + \frac{1}{2}\sin(4x) \right]_{0}^{\pi} = 2\pi

Therefore:
2π∫−ππf(x) dx=2π⋅2π=4\frac{2}{\pi} \int_{-\pi}^{\pi} f(x) \, dx = \frac{2}{\pi} \cdot 2\pi = 4

Matching for D: r


Final Summary of Matches:

  • A →\rightarrow t
  • B →\rightarrow p, r
  • C →\rightarrow q, s (or q)
  • D →\rightarrow r