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JEE Main 2020
3D Geometry
3D Geometry
Medium

Question

If the shortest distance between the straight lines 3(x1)=6(y2)=2(z1)3(x - 1) = 6(y - 2) = 2(z - 1) and 4(x2)=2(yλ)=(z3),λR4(x - 2) = 2(y - \lambda ) = (z - 3),\lambda \in R is 138{1 \over {\sqrt {38} }}, then the integral value of λ\lambda is equal to :

Options

Solution

Key Concepts and Formulas

The problem involves finding the shortest distance between two skew lines in 3D space. Skew lines are lines that are neither parallel nor intersecting.

  1. Standard Form of a Line: A straight line passing through a point (x1,y1,z1)(x_1, y_1, z_1) and having direction ratios (a,b,c)(a, b, c) can be represented in Cartesian form as xx1a=yy1b=zz1c\frac{x - x_1}{a} = \frac{y - y_1}{b} = \frac{z - z_1}{c}. In vector form, this is r=a+tb\vec{r} = \vec{a} + t\vec{b}, where a=x1i^+y1j^+z1k^\vec{a} = x_1\hat{i} + y_1\hat{j} + z_1\hat{k} is the position vector of a point on the line, and b=ai^+bj^+ck^\vec{b} = a\hat{i} + b\hat{j} + c\hat{k} is the direction vector of the line.

  2. Shortest Distance Between Two Skew Lines: For two skew lines, L1:r=a1+tb1L_1: \vec{r} = \vec{a_1} + t\vec{b_1} and L2:r=a2+sb2L_2: \vec{r} = \vec{a_2} + s\vec{b_2}, the shortest distance DD between them is given by the formula: D=(a2a1)(b1×b2)b1×b2D = \frac{|(\vec{a_2} - \vec{a_1}) \cdot (\vec{b_1} \times \vec{b_2})|}{|\vec{b_1} \times \vec{b_2}|} Here:

    • a1\vec{a_1} and a2\vec{a_2} are position vectors of points on lines L1L_1 and L2L_2 respectively.
    • b1\vec{b_1} and b2\vec{b_2} are the direction vectors of lines L1L_1 and L2L_2 respectively.
    • (a2a1)(\vec{a_2} - \vec{a_1}) is a vector connecting a point on L1L_1 to a point on L2L_2.
    • (b1×b2)(\vec{b_1} \times \vec{b_2}) is a vector perpendicular to both lines, representing the common normal direction. Its magnitude, b1×b2|\vec{b_1} \times \vec{b_2}|, is the length of this common normal vector.
    • The numerator, (a2a1)(b1×b2)|(\vec{a_2} - \vec{a_1}) \cdot (\vec{b_1} \times \vec{b_2})|, is the magnitude of the scalar triple product, which geometrically represents the volume of the parallelepiped formed by these three vectors. More importantly, it is the absolute value of the projection of the vector (a2a1)(\vec{a_2} - \vec{a_1}) onto the common normal vector (b1×b2)(\vec{b_1} \times \vec{b_2}).

Step-by-Step Solution

Step 1: Convert the Given Lines into Standard Vector Form

The first crucial step is to rewrite the given Cartesian equations of the lines into their standard symmetric form, xx1a=yy1b=zz1c\frac{x - x_1}{a} = \frac{y - y_1}{b} = \frac{z - z_1}{c}. This allows us to directly identify a point on the line (a\vec{a}) and its direction vector (b\vec{b}). Remember that the coefficients of x,y,zx, y, z in the numerator must be 1.

For Line L1L_1: The given equation is 3(x1)=6(y2)=2(z1)3(x - 1) = 6(y - 2) = 2(z - 1). To achieve the standard form, we divide each part of the equation by the Least Common Multiple (LCM) of the coefficients of the terms in the numerators (3, 6, and 2), which is 6. This normalizes the denominators to represent the direction ratios. 3(x1)6=6(y2)6=2(z1)6\frac{3(x - 1)}{6} = \frac{6(y - 2)}{6} = \frac{2(z - 1)}{6}     x12=y21=z13\implies \frac{x - 1}{2} = \frac{y - 2}{1} = \frac{z - 1}{3} From this standard form, we can identify:

  • A point on L1L_1: a1=1i^+2j^+1k^\vec{a_1} = 1\hat{i} + 2\hat{j} + 1\hat{k}.
  • The direction vector of L1L_1: b1=2i^+1j^+3k^\vec{b_1} = 2\hat{i} + 1\hat{j} + 3\hat{k}.

For Line L2L_2: The given equation is 4(x2)=2(yλ)=(z3)4(x - 2) = 2(y - \lambda ) = (z - 3). Similarly, we divide by the LCM of the coefficients (4, 2, and 1), which is 4. 4(x2)4=2(yλ)4=(z3)4\frac{4(x - 2)}{4} = \frac{2(y - \lambda)}{4} = \frac{(z - 3)}{4}     x21=yλ2=z34\implies \frac{x - 2}{1} = \frac{y - \lambda}{2} = \frac{z - 3}{4} From this standard form, we can identify:

  • A point on L2L_2: a2=2i^+λj^+3k^\vec{a_2} = 2\hat{i} + \lambda\hat{j} + 3\hat{k}.
  • The direction vector of L2L_2: b2=1i^+2j^+4k^\vec{b_2} = 1\hat{i} + 2\hat{j} + 4\hat{k}.

Step 2: Calculate the Necessary Vector Components for the Shortest Distance Formula

Now we compute the specific vector quantities required for the shortest distance formula.

2a. Calculate the vector (a2a1)(\vec{a_2} - \vec{a_1}): This vector connects a known point on L1L_1 to a known point on L2L_2. a2a1=(2i^+λj^+3k^)(1i^+2j^+1k^)\vec{a_2} - \vec{a_1} = (2\hat{i} + \lambda\hat{j} + 3\hat{k}) - (1\hat{i} + 2\hat{j} + 1\hat{k}) a2a1=(21)i^+(λ2)j^+(31)k^\vec{a_2} - \vec{a_1} = (2 - 1)\hat{i} + (\lambda - 2)\hat{j} + (3 - 1)\hat{k} a2a1=i^+(λ2)j^+2k^\vec{a_2} - \vec{a_1} = \hat{i} + (\lambda - 2)\hat{j} + 2\hat{k}

2b. Calculate the cross product (b1×b2)(\vec{b_1} \times \vec{b_2}): This vector represents the common normal to both lines, which is essential for determining the direction of the shortest distance. b1×b2=i^j^k^213124\vec{b_1} \times \vec{b_2} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 1 & 3 \\ 1 & 2 & 4 \end{vmatrix} Expanding the determinant: =i^(1432)j^(2431)+k^(2211)= \hat{i}(1 \cdot 4 - 3 \cdot 2) - \hat{j}(2 \cdot 4 - 3 \cdot 1) + \hat{k}(2 \cdot 2 - 1 \cdot 1) =i^(46)j^(83)+k^(41)= \hat{i}(4 - 6) - \hat{j}(8 - 3) + \hat{k}(4 - 1) =2i^5j^+3k^= -2\hat{i} - 5\hat{j} + 3\hat{k}

2c. Calculate the magnitude of b1×b2|\vec{b_1} \times \vec{b_2}|: This magnitude forms the denominator of the shortest distance formula. b1×b2=(2)2+(5)2+(3)2|\vec{b_1} \times \vec{b_2}| = \sqrt{(-2)^2 + (-5)^2 + (3)^2} =4+25+9=38= \sqrt{4 + 25 + 9} = \sqrt{38}

2d. Calculate the scalar triple product (a2a1)(b1×b2)(\vec{a_2} - \vec{a_1}) \cdot (\vec{b_1} \times \vec{b_2}): This scalar value forms the numerator (before taking the absolute value) and can be computed as the dot product of the vector from Step 2a and the vector from Step 2b. Alternatively, it can be calculated directly as a 3×33 \times 3 determinant with the components of the three vectors. (a2a1)(b1×b2)=1λ22213124(\vec{a_2} - \vec{a_1}) \cdot (\vec{b_1} \times \vec{b_2}) = \begin{vmatrix} 1 & \lambda - 2 & 2 \\ 2 & 1 & 3 \\ 1 & 2 & 4 \end{vmatrix} Expanding the determinant along the first row: =1(1432)(λ2)(2431)+2(2211)= 1 \cdot (1 \cdot 4 - 3 \cdot 2) - (\lambda - 2) \cdot (2 \cdot 4 - 3 \cdot 1) + 2 \cdot (2 \cdot 2 - 1 \cdot 1) =1(46)(λ2)(83)+2(41)= 1 \cdot (4 - 6) - (\lambda - 2) \cdot (8 - 3) + 2 \cdot (4 - 1) =1(2)(λ2)(5)+2(3)= 1 \cdot (-2) - (\lambda - 2) \cdot (5) + 2 \cdot (3) =25λ+10+6= -2 - 5\lambda + 10 + 6 =145λ= 14 - 5\lambda

Step 3: Apply the Shortest Distance Formula and Solve for λ\lambda

We are given that the shortest distance D=138D = \frac{1}{\sqrt{38}}. Now, we substitute all the calculated components into the shortest distance formula: D=(a2a1)(b1×b2)b1×b2D = \frac{|(\vec{a_2} - \vec{a_1}) \cdot (\vec{b_1} \times \vec{b_2})|}{|\vec{b_1} \times \vec{b_2}|} 138=145λ38\frac{1}{\sqrt{38}} = \frac{|14 - 5\lambda|}{\sqrt{38}} Since the denominators are equal and non-zero, we can equate the numerators: 145λ=1|14 - 5\lambda| = 1 To solve this absolute value equation, we consider two possible cases: Case 1: 145λ=114 - 5\lambda = 1 5λ=1415\lambda = 14 - 1 5λ=135\lambda = 13 λ=135\lambda = \frac{13}{5} Case 2: 145λ=114 - 5\lambda = -1 5λ=14+15\lambda = 14 + 1 5λ=155\lambda = 15 λ=3\lambda = 3 The problem specifically asks for the integral value of λ\lambda. Comparing the two solutions, 135\frac{13}{5} (which is 2.6) and 33, the integral value is 33.

Common Mistakes & Tips

  • Standard Form Conversion: Always ensure the coefficients of x,y,zx, y, z in the numerator are 1. If you have Axx1Ax - x_1, rewrite it as A(xx1/A)A(x - x_1/A) and divide the corresponding denominator by AA.
  • Cross Product and Determinant Calculation: Be meticulous with signs and arithmetic when calculating the cross product and the scalar triple product (determinant). A single error can propagate through the entire solution.
  • Absolute Value: Do not forget the absolute value in the shortest distance formula. Ignoring it might lead to only one solution or a negative distance, which is physically impossible.
  • Answering the Specific Question: Pay attention to what the question asks for (e.g., "integral value"). Always review your final answers against the question's requirements.

Summary

To find the integral value of λ\lambda given the shortest distance between two skew lines, we first converted the Cartesian equations of the lines into their standard vector forms to extract the point vectors (a1,a2\vec{a_1}, \vec{a_2}) and direction vectors (b1,b2\vec{b_1}, \vec{b_2}). We then calculated the necessary components: the vector connecting points on the lines (a2a1\vec{a_2} - \vec{a_1}), the common normal vector (b1×b2\vec{b_1} \times \vec{b_2}), its magnitude, and the scalar triple product. Substituting these into the shortest distance formula and solving the resulting absolute value equation yielded two possible values for λ\lambda. Finally, selecting the integral value among these solutions gave us the answer.

The integral value of λ\lambda is 3, which corresponds to option (A).

The final answer is 3\boxed{3}.

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