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JEE Main 2021
3D Geometry
3D Geometry
Hard

Question

The vector equation of the plane through the line of intersection of the planes x + y + z = 1 and 2x + 3y+ 4z = 5 which is perpendicular to the plane x – y + z = 0 is :

Options

Solution

1. Key Concepts and Formulas

This problem requires us to determine the equation of a plane that satisfies two specific conditions:

  1. It passes through the line of intersection of two given planes.
  2. It is perpendicular to a third given plane.

To achieve this, we will utilize the following fundamental concepts from 3D geometry:

  • Equation of a Plane through the Line of Intersection of Two Planes: If P1:A1x+B1y+C1z+D1=0P_1: A_1x + B_1y + C_1z + D_1 = 0 and P2:A2x+B2y+C2z+D2=0P_2: A_2x + B_2y + C_2z + D_2 = 0 are the Cartesian equations of two distinct planes, then the equation of any plane passing through their line of intersection is given by: P1+λP2=0P_1 + \lambda P_2 = 0 where λ\lambda is an arbitrary scalar constant. This equation represents a family of planes, and a specific value of λ\lambda defines the unique plane that satisfies any additional given condition.

  • Condition for Perpendicularity of Two Planes: Two planes, A1x+B1y+C1z+D1=0A_1x + B_1y + C_1z + D_1 = 0 and A2x+B2y+C2z+D2=0A_2x + B_2y + C_2z + D_2 = 0, are perpendicular if and only if their normal vectors are orthogonal. The normal vector to a plane Ax+By+Cz+D=0Ax + By + Cz + D = 0 is n=Ai^+Bj^+Ck^\vec{n} = A\hat{i} + B\hat{j} + C\hat{k}. Thus, the condition for perpendicularity is: n1n2=0A1A2+B1B2+C1C2=0\vec{n_1} \cdot \vec{n_2} = 0 \quad \Rightarrow \quad A_1A_2 + B_1B_2 + C_1C_2 = 0

  • Conversion between Cartesian and Vector Form of a Plane:

    • Cartesian to Vector: A plane given by Ax+By+Cz+D=0Ax + By + Cz + D = 0 can be expressed in vector form as r(Ai^+Bj^+Ck^)+D=0\vec{r} \cdot (A\hat{i} + B\hat{j} + C\hat{k}) + D = 0, where r=xi^+yj^+zk^\vec{r} = x\hat{i} + y\hat{j} + z\hat{k} is the position vector of any point on the plane. The vector n=Ai^+Bj^+Ck^\vec{n} = A\hat{i} + B\hat{j} + C\hat{k} is the normal vector to the plane.
    • Vector to Cartesian: Conversely, a plane given by rn+D=0\vec{r} \cdot \vec{n} + D = 0 can be written as Ax+By+Cz+D=0Ax + By + Cz + D = 0 by substituting r=xi^+yj^+zk^\vec{r} = x\hat{i} + y\hat{j} + z\hat{k} and n=Ai^+Bj^+Ck^\vec{n} = A\hat{i} + B\hat{j} + C\hat{k}.

2. Step-by-Step Solution

Step 2.1: Formulate the general equation of the required plane We are given two planes whose line of intersection defines the family of planes our desired plane belongs to. First, we write their equations in the standard Ax+By+Cz+D=0Ax+By+Cz+D=0 form:

  • Plane P1P_1: x+y+z1=0x + y + z - 1 = 0
  • Plane P2P_2: 2x+3y+4z5=02x + 3y + 4z - 5 = 0

Using the formula P1+λP2=0P_1 + \lambda P_2 = 0, the equation of any plane passing through the line of intersection of P1P_1 and P2P_2 is: (x+y+z1)+λ(2x+3y+4z5)=0(x + y + z - 1) + \lambda (2x + 3y + 4z - 5) = 0 To clearly identify the coefficients of x,y,zx, y, z and the constant term, we group them: (1+2λ)x+(1+3λ)y+(1+4λ)z(1+5λ)=0(1)(1 + 2\lambda)x + (1 + 3\lambda)y + (1 + 4\lambda)z - (1 + 5\lambda) = 0 \quad \ldots (1) This is the Cartesian equation of the general plane. Our next step is to find the specific value of λ\lambda that satisfies the second condition (perpendicularity).

Step 2.2: Identify normal vectors The normal vector to a plane Ax+By+Cz+D=0Ax + By + Cz + D = 0 is n=Ai^+Bj^+Ck^\vec{n} = A\hat{i} + B\hat{j} + C\hat{k}.

  • Normal vector to plane (1): From equation (1), the coefficients of x,y,zx, y, z are A1=(1+2λ)A_1 = (1 + 2\lambda), B1=(1+3λ)B_1 = (1 + 3\lambda), and C1=(1+4λ)C_1 = (1 + 4\lambda). So, the normal vector to our required plane is: n1=(1+2λ)i^+(1+3λ)j^+(1+4λ)k^\vec{n_1} = (1 + 2\lambda)\hat{i} + (1 + 3\lambda)\hat{j} + (1 + 4\lambda)\hat{k}

  • Normal vector to the perpendicular plane: The required plane must be perpendicular to the plane P3:xy+z=0P_3: x - y + z = 0. The coefficients of x,y,zx, y, z for P3P_3 are A2=1A_2 = 1, B2=1B_2 = -1, and C2=1C_2 = 1. So, the normal vector to P3P_3 is: n2=1i^1j^+1k^=i^j^+k^\vec{n_2} = 1\hat{i} - 1\hat{j} + 1\hat{k} = \hat{i} - \hat{j} + \hat{k}

Step 2.3: Apply the condition for perpendicularity to find λ\lambda Since plane (1) is perpendicular to P3P_3, their normal vectors n1\vec{n_1} and n2\vec{n_2} must be orthogonal. This means their dot product must be zero: n1n2=0\vec{n_1} \cdot \vec{n_2} = 0 ((1+2λ)i^+(1+3λ)j^+(1+4λ)k^)(i^j^+k^)=0((1 + 2\lambda)\hat{i} + (1 + 3\lambda)\hat{j} + (1 + 4\lambda)\hat{k}) \cdot (\hat{i} - \hat{j} + \hat{k}) = 0 Performing the dot product: (1+2λ)(1)+(1+3λ)(1)+(1+4λ)(1)=0(1 + 2\lambda)(1) + (1 + 3\lambda)(-1) + (1 + 4\lambda)(1) = 0 1+2λ13λ+1+4λ=01 + 2\lambda - 1 - 3\lambda + 1 + 4\lambda = 0 Combine the like terms: (2λ3λ+4λ)+(11+1)=0(2\lambda - 3\lambda + 4\lambda) + (1 - 1 + 1) = 0 3λ+1=03\lambda + 1 = 0 Solving for λ\lambda: 3λ=1λ=133\lambda = -1 \quad \Rightarrow \quad \lambda = -\frac{1}{3}

Step 2.4: Determine the specific plane equation Now we substitute the value of λ=13\lambda = -\frac{1}{3} back into the general equation of the plane (1): x(1+2(13))+y(1+3(13))+z(1+4(13))(1+5(13))=0x\left(1 + 2\left(-\frac{1}{3}\right)\right) + y\left(1 + 3\left(-\frac{1}{3}\right)\right) + z\left(1 + 4\left(-\frac{1}{3}\right)\right) - \left(1 + 5\left(-\frac{1}{3}\right)\right) = 0 Simplify the coefficients: x(123)+y(11)+z(143)(153)=0x\left(1 - \frac{2}{3}\right) + y\left(1 - 1\right) + z\left(1 - \frac{4}{3}\right) - \left(1 - \frac{5}{3}\right) = 0 x(13)+y(0)+z(13)(23)=0x\left(\frac{1}{3}\right) + y(0) + z\left(-\frac{1}{3}\right) - \left(-\frac{2}{3}\right) = 0 x3z3+23=0\frac{x}{3} - \frac{z}{3} + \frac{2}{3} = 0 To simplify and remove the denominators, we multiply the entire equation by 3: xz+2=0x - z + 2 = 0 This is the Cartesian equation of the required plane.

Step 2.5: Convert to vector form and match options The Cartesian equation of the plane is xz+2=0x - z + 2 = 0. To convert this to the vector form rn+D=0\vec{r} \cdot \vec{n} + D = 0, we identify the normal vector n\vec{n} and the constant DD. Here, the coefficients are A=1A=1, B=0B=0, C=1C=-1, and the constant term is D=2D=2. So, the normal vector is n=1i^+0j^1k^=i^k^\vec{n} = 1\hat{i} + 0\hat{j} - 1\hat{k} = \hat{i} - \hat{k}. The vector equation of the plane is: r(i^k^)+2=0\vec{r} \cdot (\hat{i} - \hat{k}) + 2 = 0 Comparing this result with the given options, this equation directly matches option (C).

3. Common Mistakes & Tips

  • Operator Confusion (Dot vs. Cross Product): A common mistake is to confuse the dot product (rn=d\vec{r} \cdot \vec{n} = d) which defines a plane, with a cross product (r×n=c\vec{r} \times \vec{n} = \vec{c}) which defines a line. Always remember that the equation of a plane involves a dot product with its normal vector.
  • Sign Errors with Constant Terms: Be careful when writing planes as Ax+By+Cz+D=0Ax+By+Cz+D=0. If the original plane is Ax+By+Cz=dAx+By+Cz=d, then D=dD=-d. Consistent handling of signs is crucial, especially when substituting λ\lambda into the constant part of the equation P1+λP2=0P_1 + \lambda P_2 = 0.
  • Algebraic Precision: Mistakes often occur in simplifying expressions with λ\lambda or when substituting its value back into the equation. Double-check all calculations, especially when dealing with fractions.

4. Summary

To find the equation of a plane passing through the line of intersection of two planes and perpendicular to a third plane, we first form the general equation of the plane P1+λP2=0P_1 + \lambda P_2 = 0. Then, we identify the normal vector of this general plane and the normal vector of the plane it needs to be perpendicular to. By applying the perpendicularity condition (n1n2=0\vec{n_1} \cdot \vec{n_2} = 0), we solve for the scalar λ\lambda. Substituting this value of λ\lambda back into the general equation yields the specific Cartesian equation of the required plane. Finally, this Cartesian equation is converted into its vector form rn+D=0\vec{r} \cdot \vec{n} + D = 0. Following these steps, the derived vector equation for the plane is r(i^k^)+2=0\vec{r} \cdot (\hat{i} - \hat{k}) + 2 = 0.

The final answer is A\boxed{A}.

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