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JEE Main 2023
3D Geometry
3D Geometry
Hard

Question

Let the line L\mathrm{L} intersect the lines x2=y=z1,2(x+1)=2(y1)=z+1x-2=-y=z-1,2(x+1)=2(y-1)=z+1 and be parallel to the line x23=y11=z22\frac{x-2}{3}=\frac{y-1}{1}=\frac{z-2}{2}. Then which of the following points lies on L\mathrm{L} ?

Options

Solution

Key Concepts and Formulas

  • Parametric Equation of a Line: A line passing through a point (x0,y0,z0)(x_0, y_0, z_0) with a direction vector a,b,c\langle a, b, c \rangle can be represented parametrically as x=x0+aλx = x_0 + a\lambda, y=y0+bλy = y_0 + b\lambda, z=z0+cλz = z_0 + c\lambda, where λ\lambda is a scalar parameter. This form is crucial for representing any general point on a line.
  • Direction Vector of a Line: The direction vector of a line passing through two points P1(x1,y1,z1)P_1(x_1, y_1, z_1) and P2(x2,y2,z2)P_2(x_2, y_2, z_2) is given by P1P2=x2x1,y2y1,z2z1\vec{P_1P_2} = \langle x_2-x_1, y_2-y_1, z_2-z_1 \rangle. Also, for a line in symmetric form xx0a=yy0b=zz0c\frac{x-x_0}{a} = \frac{y-y_0}{b} = \frac{z-z_0}{c}, the direction vector is a,b,c\langle a, b, c \rangle.
  • Parallel Lines: Two lines are parallel if and only if their direction vectors are proportional. That is, if d1\vec{d_1} and d2\vec{d_2} are the direction vectors of two parallel lines, then d1=kd2\vec{d_1} = k \cdot \vec{d_2} for some non-zero scalar kk.
  • Equation of a Line (Point-Direction Form): Given a point (x0,y0,z0)(x_0, y_0, z_0) on the line and its direction vector a,b,c\langle a, b, c \rangle, the symmetric equation of the line is xx0a=yy0b=zz0c\frac{x-x_0}{a} = \frac{y-y_0}{b} = \frac{z-z_0}{c}.

Step-by-Step Solution

Step 1: Convert the given lines into their parametric forms. To find the line L, we first need to express the two lines it intersects (L1L_1 and L2L_2) in a way that allows us to represent any point on them using a parameter. This is best done using parametric equations.

  • Line L1L_1: x2=y=z1x-2 = -y = z-1 First, write it in standard symmetric form: L1:x21=y01=z11L_1: \frac{x-2}{1} = \frac{y-0}{-1} = \frac{z-1}{1} Now, set each ratio equal to a parameter, say λ\lambda, to get the parametric form for any point P1P_1 on L1L_1: P1(λ)=(λ+2,λ,λ+1)P_1(\lambda) = (\lambda+2, -\lambda, \lambda+1) Reasoning: The parametric form allows us to express the coordinates of any point on L1L_1 using a single variable λ\lambda. This is essential for defining the intersection point of LL with L1L_1.

  • Line L2L_2: 2(x+1)=2(y1)=z+12(x+1) = 2(y-1) = z+1 To convert to standard symmetric form, we divide the first two parts by 2: L2:x+11/2=y11/2=z+11L_2: \frac{x+1}{1/2} = \frac{y-1}{1/2} = \frac{z+1}{1} Set each ratio equal to a parameter, say μ\mu, to get the parametric form for any point P2P_2 on L2L_2: P2(μ)=(μ21,μ2+1,μ1)P_2(\mu) = \left(\frac{\mu}{2}-1, \frac{\mu}{2}+1, \mu-1\right) Reasoning: Similar to L1L_1, this parametric representation for L2L_2 will allow us to define the intersection point of LL with L2L_2.

Step 2: Determine the direction vector of line L. Line L intersects L1L_1 at a point P1(λ)P_1(\lambda) and L2L_2 at a point P2(μ)P_2(\mu). Therefore, the vector connecting these two points, P1P2\vec{P_1P_2}, must be a direction vector for line L. We calculate P1P2=P2P1\vec{P_1P_2} = P_2 - P_1: P1P2=(μ21)(λ+2),(μ2+1)(λ),(μ1)(λ+1)\vec{P_1P_2} = \left\langle \left(\frac{\mu}{2}-1\right) - (\lambda+2), \left(\frac{\mu}{2}+1\right) - (-\lambda), (\mu-1) - (\lambda+1) \right\rangle P1P2=μ2λ3,μ2+λ+1,μλ2\vec{P_1P_2} = \left\langle \frac{\mu}{2} - \lambda - 3, \frac{\mu}{2} + \lambda + 1, \mu - \lambda - 2 \right\rangle Reasoning: If a line passes through two specific points, the vector connecting these two points lies along the line and thus serves as its direction vector.

Step 3: Apply the parallelism condition. Line L is given to be parallel to the line x23=y11=z22\frac{x-2}{3}=\frac{y-1}{1}=\frac{z-2}{2}. The direction vector of this parallel line (let's call it LPL_P) is dP=3,1,2\vec{d_P} = \langle 3, 1, 2 \rangle. Since line L is parallel to LPL_P, their direction vectors must be proportional. This means P1P2\vec{P_1P_2} must be a scalar multiple of dP\vec{d_P}. Let kk be the constant of proportionality: P1P2=kdP\vec{P_1P_2} = k \cdot \vec{d_P} Equating the components gives us a system of proportions: μ2λ33=μ2+λ+11=μλ22\frac{\frac{\mu}{2} - \lambda - 3}{3} = \frac{\frac{\mu}{2} + \lambda + 1}{1} = \frac{\mu - \lambda - 2}{2} Reasoning: This step translates the geometric condition of parallelism into algebraic equations involving our parameters λ\lambda and μ\mu, which we can then solve.

Step 4: Solve the system of equations for λ\lambda and μ\mu. From the proportionality in Step 3, we can form two independent linear equations:

  • Equation (1): Equating the first two ratios: μ2λ3=3(μ2+λ+1)\frac{\mu}{2} - \lambda - 3 = 3 \left( \frac{\mu}{2} + \lambda + 1 \right) μ2λ3=3μ2+3λ+3\frac{\mu}{2} - \lambda - 3 = \frac{3\mu}{2} + 3\lambda + 3 Multiply by 2 to clear fractions: μ2λ6=3μ+6λ+6\mu - 2\lambda - 6 = 3\mu + 6\lambda + 6 Rearrange terms: 12=2μ+8λ-12 = 2\mu + 8\lambda μ+4λ=6(Eq. A)\mu + 4\lambda = -6 \quad \text{(Eq. A)}

  • Equation (2): Equating the second and third ratios: μ2+λ+1=μλ22\frac{\mu}{2} + \lambda + 1 = \frac{\mu - \lambda - 2}{2} Multiply by 2 to clear fractions: μ+2λ+2=μλ2\mu + 2\lambda + 2 = \mu - \lambda - 2 Rearrange terms: 2λ+2=λ22\lambda + 2 = -\lambda - 2 3λ=43\lambda = -4 λ=43\lambda = -\frac{4}{3}

Now, substitute the value of λ\lambda into Eq. A: μ+4(43)=6\mu + 4\left(-\frac{4}{3}\right) = -6 μ163=6\mu - \frac{16}{3} = -6 μ=6+163\mu = -6 + \frac{16}{3} μ=183+163\mu = -\frac{18}{3} + \frac{16}{3} μ=23\mu = -\frac{2}{3} Reasoning: Solving these equations gives us the unique values of λ\lambda and μ\mu that define the specific intersection points P1P_1 and P2P_2 on L1L_1 and L2L_2 respectively, such that the line connecting them is parallel to LPL_P.

Step 5: Determine the equation of line L. We have found λ=43\lambda = -\frac{4}{3} and μ=23\mu = -\frac{2}{3}. We can use either P1P_1 or P2P_2 as a point on line L. Let's use P1P_1. Substitute λ=43\lambda = -\frac{4}{3} into the parametric form of P1(λ)P_1(\lambda): P1=(43+2,(43),43+1)P_1 = \left(-\frac{4}{3}+2, -(-\frac{4}{3}), -\frac{4}{3}+1\right) P1=(4+63,43,4+33)P_1 = \left(\frac{-4+6}{3}, \frac{4}{3}, \frac{-4+3}{3}\right) P1=(23,43,13)P_1 = \left(\frac{2}{3}, \frac{4}{3}, -\frac{1}{3}\right) The direction vector of line L is dL=dP=3,1,2\vec{d_L} = \vec{d_P} = \langle 3, 1, 2 \rangle. Using point P1P_1 and direction vector dL\vec{d_L}, the symmetric equation of line L is: L:x233=y431=z(13)2L: \frac{x - \frac{2}{3}}{3} = \frac{y - \frac{4}{3}}{1} = \frac{z - (-\frac{1}{3})}{2} L:x233=y431=z+132L: \frac{x - \frac{2}{3}}{3} = \frac{y - \frac{4}{3}}{1} = \frac{z + \frac{1}{3}}{2} Reasoning: With a specific point on the line and its direction vector, we can uniquely write the equation of the line.

Step 6: Check the given options. To find which point lies on line L, we substitute the coordinates of each option into the equation of L and check if all three ratios are equal.

Let's check option (A) (13,1,1)\left(-\frac{1}{3}, 1, -1\right): Substitute x=13,y=1,z=1x = -\frac{1}{3}, y = 1, z = -1 into the equation of L: 13233=1431=1+132\frac{-\frac{1}{3} - \frac{2}{3}}{3} = \frac{1 - \frac{4}{3}}{1} = \frac{-1 + \frac{1}{3}}{2} 333=3431=3+132\frac{-\frac{3}{3}}{3} = \frac{\frac{3-4}{3}}{1} = \frac{\frac{-3+1}{3}}{2} 13=13=232\frac{-1}{3} = -\frac{1}{3} = \frac{-\frac{2}{3}}{2} 13=13=13-\frac{1}{3} = -\frac{1}{3} = -\frac{1}{3} All three ratios are equal to 13-\frac{1}{3}. Therefore, point (A) lies on line L. Reasoning: A point lies on a line if and only if its coordinates satisfy the line's equation.


Common Mistakes & Tips

  • Converting to Standard Form: Be extremely careful when converting lines like x2=y=z1x-2=-y=z-1 or 2(x+1)=2(y1)=z+12(x+1)=2(y-1)=z+1 to standard symmetric form. Pay attention to signs and coefficients (e.g., y-y becomes y01\frac{y-0}{-1}, and 2(x+1)2(x+1) becomes x+11/2\frac{x+1}{1/2} or, by multiplying through by 2, x+11\frac{x+1}{1}).
  • Algebraic Errors: The most common errors occur during the solution of the system of linear equations for λ\lambda and μ\mu. Fractions often complicate calculations, so double-check each step.
  • Choosing the Correct Direction Vector: Remember that the direction vector of line L is given by the line it's parallel to (dP\vec{d_P}), not necessarily the vector P1P2\vec{P_1P_2} itself, although P1P2\vec{P_1P_2} is proportional to dP\vec{d_P}. Using dP\vec{d_P} ensures the simplest form for the direction vector.

Summary

This problem combined several fundamental concepts of 3D geometry to find the equation of a specific line. We began by converting the intersecting lines into parametric forms to represent general points on them. Then, we formed a vector connecting these general points, which served as a direction vector for the desired line. By applying the parallelism condition with the third given line, we set up and solved a system of equations to find the precise values of the parameters. These parameters allowed us to determine a specific point on the line L. Finally, using this point and the known direction vector, we wrote the equation of line L and verified which of the given options lay on it. This systematic approach ensures all conditions are met, leading to the correct answer.

The final answer is (13,1,1)\boxed{\left(-\frac{1}{3}, 1,-1\right)}, which corresponds to option (A).

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