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JEE Main 2023
3D Geometry
3D Geometry
Hard

Question

Let P1\mathrm{P}_{1} be the plane 3xy7z=113 x-y-7 z=11 and P2\mathrm{P}_{2} be the plane passing through the points (2,1,0),(2,0,1)(2,-1,0),(2,0,-1), and (5,1,1)(5,1,1). If the foot of the perpendicular drawn from the point (7,4,1)(7,4,-1) on the line of intersection of the planes P1P_{1} and P2P_{2} is (α,β,γ)(\alpha, \beta, \gamma), then α+β+γ\alpha+\beta+\gamma is equal to ___________.

Answer: 2

Solution

This problem requires us to find the foot of a perpendicular from a given point to a line, where the line itself is the intersection of two planes. We will systematically approach this using concepts from 3D geometry.

1. Key Concepts and Formulas

  • Equation of a Plane: A plane can be defined by a point it passes through and its normal vector. If the plane passes through points (x1,y1,z1)(x_1, y_1, z_1), (x2,y2,z2)(x_2, y_2, z_2), and (x3,y3,z3)(x_3, y_3, z_3), its equation can be found using the determinant form or by finding two vectors in the plane, taking their cross product to get the normal vector, and then using the point-normal form.
  • Equation of a Line of Intersection: The direction vector of the line of intersection of two planes is perpendicular to both plane normal vectors. Thus, it can be found by taking the cross product of the normal vectors of the two planes. A point on the line can be found by setting one variable to zero (or any constant) in both plane equations and solving for the other two.
  • Foot of the Perpendicular from a Point to a Line: If AA is the given point and LL is the line with direction vector v\vec{v}, any point FF on LL can be expressed parametrically. The vector AF\vec{AF} (from point AA to point FF) must be perpendicular to the direction vector v\vec{v} of the line. Therefore, their dot product AFv\vec{AF} \cdot \vec{v} must be zero. This condition allows us to find the parameter value for FF, and subsequently its coordinates.

2. Step-by-Step Solution

Step 1: Find the equation of Plane P2P_2.

  • What we are doing: We need the algebraic equation of plane P2P_2 to later find its intersection with P1P_1.
  • Why: The line of intersection requires the equations of both planes.
  • Math: Plane P2P_2 passes through points B(2,1,0)B(2,-1,0), C(2,0,1)C(2,0,-1), and D(5,1,1)D(5,1,1). First, we find two vectors lying in the plane: BC=CB=(22,0(1),10)=(0,1,1)\vec{BC} = C - B = (2-2, 0-(-1), -1-0) = (0, 1, -1) BD=DB=(52,1(1),10)=(3,2,1)\vec{BD} = D - B = (5-2, 1-(-1), 1-0) = (3, 2, 1) The normal vector n2\vec{n_2} to plane P2P_2 is the cross product of BC\vec{BC} and BD\vec{BD}: n2=BC×BD=ijk011321\vec{n_2} = \vec{BC} \times \vec{BD} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ 0 & 1 & -1 \\ 3 & 2 & 1 \end{vmatrix} n2=i((1)(1)(1)(2))j((0)(1)(1)(3))+k((0)(2)(1)(3))\vec{n_2} = \mathbf{i}((1)(1) - (-1)(2)) - \mathbf{j}((0)(1) - (-1)(3)) + \mathbf{k}((0)(2) - (1)(3)) n2=i(1+2)j(0+3)+k(03)=(3,3,3)\vec{n_2} = \mathbf{i}(1+2) - \mathbf{j}(0+3) + \mathbf{k}(0-3) = (3, -3, -3) We can use a simpler normal vector parallel to (3,3,3)(3,-3,-3), which is (1,1,1)(1,-1,-1). So, we use n2=(1,1,1)\vec{n_2} = (1, -1, -1). Using the point-normal form with point B(2,1,0)B(2,-1,0) and n2=(1,1,1)\vec{n_2}=(1,-1,-1): 1(x2)1(y(1))1(z0)=01(x-2) - 1(y-(-1)) - 1(z-0) = 0 x2(y+1)z=0x-2 - (y+1) - z = 0 xyz3=0x - y - z - 3 = 0 Thus, the equation of plane P2P_2 is xyz=3x - y - z = 3.

Step 2: Find the equation of the Line of Intersection (LL) of P1P_1 and P2P_2.

  • What we are doing: We are determining the parametric equation of the line where the two planes P1P_1 and P2P_2 intersect.

  • Why: The foot of the perpendicular will lie on this line, so its equation is essential.

  • Math: The equations of the two planes are: P1:3xy7z=11P_1: 3x - y - 7z = 11 (Normal vector n1=(3,1,7)\vec{n_1} = (3, -1, -7)) P2:xyz=3P_2: x - y - z = 3 (Normal vector n2=(1,1,1)\vec{n_2} = (1, -1, -1)) The direction vector v\vec{v} of the line of intersection is perpendicular to both n1\vec{n_1} and n2\vec{n_2}. We find it using their cross product: v=n1×n2=ijk317111\vec{v} = \vec{n_1} \times \vec{n_2} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ 3 & -1 & -7 \\ 1 & -1 & -1 \end{vmatrix} v=i((1)(1)(7)(1))j((3)(1)(7)(1))+k((3)(1)(1)(1))\vec{v} = \mathbf{i}((-1)(-1) - (-7)(-1)) - \mathbf{j}((3)(-1) - (-7)(1)) + \mathbf{k}((3)(-1) - (-1)(1)) v=i(17)j(3+7)+k(3+1)\vec{v} = \mathbf{i}(1-7) - \mathbf{j}(-3+7) + \mathbf{k}(-3+1) v=(6,4,2)\vec{v} = (-6, -4, -2) We can use a simpler direction vector parallel to (6,4,2)(-6,-4,-2), which is (3,2,1)(3,2,1). So, let v=(3,2,1)\vec{v} = (3,2,1).

    Next, we need a point on the line of intersection. We can find this by setting one coordinate to zero (e.g., z=0z=0) in both plane equations and solving for xx and yy: For z=0z=0: 3xy=11(1)3x - y = 11 \quad (1) xy=3(2)x - y = 3 \quad (2) Subtracting equation (2) from equation (1): (3xy)(xy)=113(3x - y) - (x - y) = 11 - 3 2x=8    x=42x = 8 \implies x = 4 Substitute x=4x=4 into equation (2): 4y=3    y=14 - y = 3 \implies y = 1 So, a point on the line of intersection is P0(4,1,0)P_0(4,1,0). The parametric equation of the line of intersection LL is: x=4+3tx = 4 + 3t y=1+2ty = 1 + 2t z=tz = t or r(t)=(4+3t,1+2t,t)\vec{r}(t) = (4+3t, 1+2t, t).

Step 3: Find the foot of the perpendicular F(α,β,γ)F(\alpha, \beta, \gamma) from point A(7,4,1)A(7,4,-1) to line LL.

  • What we are doing: We are identifying the specific point on line LL that is closest to point AA.
  • Why: This point is defined as the foot of the perpendicular, and its coordinates are needed to calculate α+β+γ\alpha+\beta+\gamma.
  • Math: Let F(α,β,γ)F(\alpha, \beta, \gamma) be the foot of the perpendicular from A(7,4,1)A(7,4,-1) to the line LL. Any point on line LL can be represented as F(4+3t,1+2t,t)F(4+3t, 1+2t, t) for some scalar tt. The vector AF\vec{AF} connects point A(7,4,1)A(7,4,-1) to point F(4+3t,1+2t,t)F(4+3t, 1+2t, t): AF=(4+3t7,1+2t4,t(1))\vec{AF} = (4+3t - 7, 1+2t - 4, t - (-1)) AF=(3t3,2t3,t+1)\vec{AF} = (3t-3, 2t-3, t+1) The direction vector of the line LL is v=(3,2,1)\vec{v} = (3,2,1). Since AF\vec{AF} must be perpendicular to v\vec{v}, their dot product must be zero: AFv=0\vec{AF} \cdot \vec{v} = 0 (3t3)(3)+(2t3)(2)+(t+1)(1)=0(3t-3)(3) + (2t-3)(2) + (t+1)(1) = 0 9t9+4t6+t+1=09t - 9 + 4t - 6 + t + 1 = 0 14t14=014t - 14 = 0 14t=1414t = 14 t=1t = 1 Now substitute t=1t=1 back into the coordinates of FF: α=4+3(1)=7\alpha = 4 + 3(1) = 7 β=1+2(1)=3\beta = 1 + 2(1) = 3 γ=1\gamma = 1 So, the foot of the perpendicular is F(7,3,1)F(7,3,1).

Step 4: Calculate α+β+γ\alpha+\beta+\gamma.

  • What we are doing: Summing the coordinates of the foot of the perpendicular.
  • Why: This is the final value requested by the problem.
  • Math: α+β+γ=7+3+1=11\alpha+\beta+\gamma = 7+3+1 = 11

Common Mistakes & Tips

  • Sign Errors in Cross Products: Be very careful with signs when calculating cross products for normal or direction vectors. A single sign error can propagate through the entire problem.
  • Arithmetic Errors: Double-check additions, subtractions, and multiplications, especially when dealing with negative numbers. A small arithmetic mistake can lead to an incorrect value for tt.
  • Choosing a Point on the Line: When finding a point on the line of intersection, try setting z=0z=0 (or x=0x=0 or y=0y=0) and solve for the other two variables. If this results in a system with no solution or an undefined point, choose a different variable to set to zero.
  • Perpendicularity Condition: Remember that the vector from the external point to the foot of the perpendicular on the line must be orthogonal to the direction vector of the line. This is the key to finding the parameter tt.

Summary

We first determined the equation of plane P2P_2 using the three given points and found its normal vector. Then, we found the direction vector of the line of intersection of P1P_1 and P2P_2 by taking the cross product of their normal vectors, and identified a point on this line. This allowed us to write the parametric equation of the line of intersection. Finally, we used the condition that the vector from the given point AA to the foot of the perpendicular FF is orthogonal to the line's direction vector to solve for the parameter tt. Substituting tt back into the line's equation gave us the coordinates of F(α,β,γ)F(\alpha, \beta, \gamma). The sum α+β+γ\alpha+\beta+\gamma was calculated as 7+3+1=117+3+1=11.

The final answer is 11\boxed{11}.

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