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JEE Main 2019
3D Geometry
3D Geometry
Medium

Question

If the angel θ\theta between the line x+11=y12=z22{{x + 1} \over 1} = {{y - 1} \over 2} = {{z - 2} \over 2} and the plane 2xy+λz+4=02x - y + \sqrt \lambda \,\,z + 4 = 0 is such that sinθ=13\sin \,\,\theta = {1 \over 3} then value of λ\lambda is :

Options

Solution

Key Concepts and Formulas

  • Angle Between a Line and a Plane: The angle θ\theta between a line with direction vector b\vec{b} and a plane with normal vector n\vec{n} is given by the formula: sinθ=bnbn\sin \theta = \frac{|\vec{b} \cdot \vec{n}|}{|\vec{b}| |\vec{n}|} This formula is derived from the fact that the angle θ\theta between the line and the plane is complementary to the angle ϕ\phi between the line and the plane's normal vector (i.e., θ=90ϕ\theta = 90^\circ - \phi), and thus sinθ=cosϕ\sin \theta = \cos \phi.
  • Direction Vector of a Line: For a line expressed in symmetric form xx1a=yy1b=zz1c\frac{x - x_1}{a} = \frac{y - y_1}{b} = \frac{z - z_1}{c}, its direction vector is b=ai^+bj^+ck^\vec{b} = a\hat{i} + b\hat{j} + c\hat{k}.
  • Normal Vector of a Plane: For a plane expressed in general form Ax+By+Cz+D=0Ax + By + Cz + D = 0, its normal vector is n=Ai^+Bj^+Ck^\vec{n} = A\hat{i} + B\hat{j} + C\hat{k}.

Step-by-Step Solution

Step 1: Identify the Direction Vector of the Line

We begin by extracting the direction vector from the given equation of the line. The line is given by: x+11=y12=z22\frac{x + 1}{1} = \frac{y - 1}{2} = \frac{z - 2}{2} Comparing this with the standard symmetric form xx1a=yy1b=zz1c\frac{x - x_1}{a} = \frac{y - y_1}{b} = \frac{z - z_1}{c}, we can identify the direction ratios (a,b,c)(a, b, c) as (1,2,2)(1, 2, 2). Therefore, the direction vector of the line is: b=1i^+2j^+2k^\vec{b} = 1\hat{i} + 2\hat{j} + 2\hat{k}

Step 2: Identify the Normal Vector of the Plane

Next, we extract the normal vector from the given equation of the plane. The plane is given by: 2xy+λz+4=02x - y + \sqrt{\lambda}z + 4 = 0 Comparing this with the standard general form Ax+By+Cz+D=0Ax + By + Cz + D = 0, we identify the coefficients of x,y,zx, y, z as A=2A=2, B=1B=-1, and C=λC=\sqrt{\lambda}. Therefore, the normal vector to the plane is: n=2i^1j^+λk^\vec{n} = 2\hat{i} - 1\hat{j} + \sqrt{\lambda}\hat{k} Note: For λ\sqrt{\lambda} to be a real number, it is implicitly assumed that λ0\lambda \ge 0. This will be important for simplifying absolute values later.

Step 3: Calculate the Dot Product of the Vectors

Now, we compute the dot product of the direction vector of the line (b\vec{b}) and the normal vector of the plane (n\vec{n}). The dot product is the sum of the products of their corresponding components: bn=(1)(2)+(2)(1)+(2)(λ)\vec{b} \cdot \vec{n} = (1)(2) + (2)(-1) + (2)(\sqrt{\lambda}) bn=22+2λ\vec{b} \cdot \vec{n} = 2 - 2 + 2\sqrt{\lambda} bn=2λ\vec{b} \cdot \vec{n} = 2\sqrt{\lambda}

Step 4: Calculate the Magnitudes of the Vectors

We need the magnitudes (lengths) of both vectors for the formula. The magnitude of a vector pi^+qj^+rk^p\hat{i} + q\hat{j} + r\hat{k} is p2+q2+r2\sqrt{p^2 + q^2 + r^2}.

  • Magnitude of b\vec{b}: b=12+22+22=1+4+4=9=3|\vec{b}| = \sqrt{1^2 + 2^2 + 2^2} = \sqrt{1 + 4 + 4} = \sqrt{9} = 3

  • Magnitude of n\vec{n}: n=22+(1)2+(λ)2=4+1+λ=5+λ|\vec{n}| = \sqrt{2^2 + (-1)^2 + (\sqrt{\lambda})^2} = \sqrt{4 + 1 + \lambda} = \sqrt{5 + \lambda}

Step 5: Substitute into the Formula and Solve for λ\lambda

We are given that the angle θ\theta between the line and the plane satisfies sinθ=13\sin \theta = \frac{1}{3}. We substitute the calculated values into the formula sinθ=bnbn\sin \theta = \frac{|\vec{b} \cdot \vec{n}|}{|\vec{b}| |\vec{n}|}: 13=2λ35+λ\frac{1}{3} = \frac{|2\sqrt{\lambda}|}{3 \cdot \sqrt{5 + \lambda}} Since we established that λ0\lambda \ge 0, 2λ2\sqrt{\lambda} will always be non-negative, so 2λ=2λ|2\sqrt{\lambda}| = 2\sqrt{\lambda}. 13=2λ35+λ\frac{1}{3} = \frac{2\sqrt{\lambda}}{3\sqrt{5 + \lambda}} We can cancel the '3' from both denominators: 1=2λ5+λ1 = \frac{2\sqrt{\lambda}}{\sqrt{5 + \lambda}} Rearrange the equation to isolate the square roots: 5+λ=2λ\sqrt{5 + \lambda} = 2\sqrt{\lambda} To eliminate the square roots and solve for λ\lambda, we square both sides of the equation: (5+λ)2=(2λ)2(\sqrt{5 + \lambda})^2 = (2\sqrt{\lambda})^2 5+λ=4λ5 + \lambda = 4\lambda Now, we solve for λ\lambda: 5=4λλ5 = 4\lambda - \lambda 5=3λ5 = 3\lambda λ=53\lambda = \frac{5}{3}

Step 6: Verify the Solution

It is a good practice to verify solutions, especially after squaring both sides of an equation, to ensure no extraneous solutions have been introduced. Substitute λ=53\lambda = \frac{5}{3} back into the equation before squaring, i.e., 5+λ=2λ\sqrt{5 + \lambda} = 2\sqrt{\lambda}: 5+53=253\sqrt{5 + \frac{5}{3}} = 2\sqrt{\frac{5}{3}} 15+53=253\sqrt{\frac{15+5}{3}} = 2\sqrt{\frac{5}{3}} 203=253\sqrt{\frac{20}{3}} = 2\sqrt{\frac{5}{3}} We know that 203=453=453=253\sqrt{\frac{20}{3}} = \sqrt{4 \cdot \frac{5}{3}} = \sqrt{4} \cdot \sqrt{\frac{5}{3}} = 2\sqrt{\frac{5}{3}}. 253=2532\sqrt{\frac{5}{3}} = 2\sqrt{\frac{5}{3}} The solution is consistent. Also, λ=5/3\lambda = 5/3 satisfies the condition λ0\lambda \ge 0.

Common Mistakes & Tips

  • Angle Confusion: Be careful not to confuse the angle θ\theta between the line and the plane with the angle ϕ\phi between the line and the normal to the plane. The formula cosϕ=bnbn\cos \phi = \frac{|\vec{b} \cdot \vec{n}|}{|\vec{b}| |\vec{n}|} is for ϕ\phi, whereas sinθ=bnbn\sin \theta = \frac{|\vec{b} \cdot \vec{n}|}{|\vec{b}| |\vec{n}|} is for θ\theta. Remember that θ=90ϕ\theta = 90^\circ - \phi.
  • Absolute Value: Always include the absolute value in the numerator, bn|\vec{b} \cdot \vec{n}|, as the angle θ\theta between a line and a plane is conventionally taken as an acute angle (0θ900 \le \theta \le 90^\circ), for which sinθ0\sin \theta \ge 0.
  • Verification after Squaring: When you square both sides of an equation to remove square roots, always check your final answer in the original equation (or the equation just before squaring) to ensure it is a valid solution and not an extraneous one.

Summary

This problem involved finding an unknown parameter λ\lambda by utilizing the formula for the angle between a line and a plane. We systematically extracted the direction vector of the line and the normal vector of the plane from their given equations. We then computed their dot product and magnitudes, substituting these values into the sinθ\sin \theta formula along with the given value of sinθ\sin \theta. Solving the resulting algebraic equation, which involved squaring both sides, yielded the value of λ\lambda. Finally, the solution was verified to ensure its validity.

The final answer is 53\boxed{{5 \over 3}}, which corresponds to option (A).

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