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JEE Main 2023
Vector Algebra
Vector Algebra
Medium

Question

For p > 0, a vector v2=2i^+(p+1)j^{\overrightarrow v _2} = 2\widehat i + (p + 1)\widehat j is obtained by rotating the vector v1=3pi^+j^{\overrightarrow v _1} = \sqrt 3 p\widehat i + \widehat j by an angle θ\theta about origin in counter clockwise direction. If tanθ=(α32)(43+3)\tan \theta = {{\left( {\alpha \sqrt 3 - 2} \right)} \over {\left( {4\sqrt 3 + 3} \right)}}, then the value of α\alpha is equal to _____________.

Answer: 1

Solution

Key Concepts and Formulas

  • Vector Magnitude: The magnitude of a vector v=xi^+yj^\overrightarrow{v} = x\widehat{i} + y\widehat{j} is v=x2+y2|\overrightarrow{v}| = \sqrt{x^2 + y^2}. Rotation about the origin preserves the magnitude of a vector.
  • Dot Product: For vectors A\overrightarrow{A} and B\overrightarrow{B}, AB=ABcosθ\overrightarrow{A} \cdot \overrightarrow{B} = |\overrightarrow{A}| |\overrightarrow{B}| \cos \theta, where θ\theta is the angle between them.
  • Cross Product (2D interpretation): For vectors v1=x1i^+y1j^\overrightarrow{v_1} = x_1\widehat{i} + y_1\widehat{j} and v2=x2i^+y2j^\overrightarrow{v_2} = x_2\widehat{i} + y_2\widehat{j}, the zz-component of the cross product is x1y2x2y1x_1y_2 - x_2y_1. If this value is positive, the rotation from v1\overrightarrow{v_1} to v2\overrightarrow{v_2} is counter-clockwise, and sinθ=x1y2x2y1v1v2\sin \theta = \frac{x_1y_2 - x_2y_1}{|\overrightarrow{v_1}||\overrightarrow{v_2}|}.
  • Trigonometric Identity: sin2θ+cos2θ=1\sin^2 \theta + \cos^2 \theta = 1.
  • Simplification of Nested Radicals: A±2B=x±y\sqrt{A \pm 2\sqrt{B}} = \sqrt{x} \pm \sqrt{y}, where x+y=Ax+y=A and xy=Bxy=B.

Step-by-Step Solution

Step 1: Determine the value of 'p' by equating vector magnitudes.

The problem states that vector v2\overrightarrow{v_2} is obtained by rotating vector v1\overrightarrow{v_1} about the origin. Rotation about the origin is an isometry, meaning it preserves the length (magnitude) of the vector. Therefore, v1=v2|\overrightarrow{v_1}| = |\overrightarrow{v_2}|.

Given vectors: v1=3pi^+j^\overrightarrow{v_1} = \sqrt{3}p\widehat{i} + \widehat{j} v2=2i^+(p+1)j^\overrightarrow{v_2} = 2\widehat{i} + (p+1)\widehat{j}

Calculate the square of the magnitudes: v12=(3p)2+(1)2=3p2+1|\overrightarrow{v_1}|^2 = (\sqrt{3}p)^2 + (1)^2 = 3p^2 + 1 v22=(2)2+(p+1)2=4+(p2+2p+1)=p2+2p+5|\overrightarrow{v_2}|^2 = (2)^2 + (p+1)^2 = 4 + (p^2 + 2p + 1) = p^2 + 2p + 5

Equate the squared magnitudes: 3p2+1=p2+2p+53p^2 + 1 = p^2 + 2p + 5

Rearrange into a quadratic equation: 2p22p4=02p^2 - 2p - 4 = 0

Divide by 2: p2p2=0p^2 - p - 2 = 0

Factor the quadratic equation: (p2)(p+1)=0(p-2)(p+1) = 0

This yields two possible values for pp: p=2p=2 and p=1p=-1. The problem states that p>0p > 0. Therefore, we select p=2p=2.

Step 2: Substitute p=2p=2 into the vectors and calculate cosθ\cos \theta.

Now that we have the value of pp, we can write the explicit forms of the vectors.

v1=3(2)i^+j^=23i^+j^\overrightarrow{v_1} = \sqrt{3}(2)\widehat{i} + \widehat{j} = 2\sqrt{3}\widehat{i} + \widehat{j} v2=2i^+(2+1)j^=2i^+3j^\overrightarrow{v_2} = 2\widehat{i} + (2+1)\widehat{j} = 2\widehat{i} + 3\widehat{j}

Calculate the magnitudes of these vectors: v1=(23)2+12=12+1=13|\overrightarrow{v_1}| = \sqrt{(2\sqrt{3})^2 + 1^2} = \sqrt{12 + 1} = \sqrt{13} v2=22+32=4+9=13|\overrightarrow{v_2}| = \sqrt{2^2 + 3^2} = \sqrt{4 + 9} = \sqrt{13} As expected, the magnitudes are equal.

Calculate the dot product v1v2\overrightarrow{v_1} \cdot \overrightarrow{v_2}: v1v2=(23)(2)+(1)(3)=43+3\overrightarrow{v_1} \cdot \overrightarrow{v_2} = (2\sqrt{3})(2) + (1)(3) = 4\sqrt{3} + 3

Use the dot product formula to find cosθ\cos \theta: cosθ=v1v2v1v2=43+31313=43+313\cos \theta = \frac{\overrightarrow{v_1} \cdot \overrightarrow{v_2}}{|\overrightarrow{v_1}| |\overrightarrow{v_2}|} = \frac{4\sqrt{3} + 3}{\sqrt{13} \cdot \sqrt{13}} = \frac{4\sqrt{3} + 3}{13}

Step 3: Determine sinθ\sin \theta using the direction of rotation and calculate tanθ\tan \theta.

The problem specifies that v2\overrightarrow{v_2} is obtained by rotating v1\overrightarrow{v_1} by an angle θ\theta in the counter-clockwise direction. For 2D vectors v1=x1i^+y1j^\overrightarrow{v_1} = x_1\widehat{i} + y_1\widehat{j} and v2=x2i^+y2j^\overrightarrow{v_2} = x_2\widehat{i} + y_2\widehat{j}, the sine of the counter-clockwise angle θ\theta is given by sinθ=x1y2x2y1v1v2\sin \theta = \frac{x_1y_2 - x_2y_1}{|\overrightarrow{v_1}||\overrightarrow{v_2}|}.

Using v1=23i^+j^\overrightarrow{v_1} = 2\sqrt{3}\widehat{i} + \widehat{j} and v2=2i^+3j^\overrightarrow{v_2} = 2\widehat{i} + 3\widehat{j}: x1=23,y1=1x_1 = 2\sqrt{3}, \quad y_1 = 1 x2=2,y2=3x_2 = 2, \quad y_2 = 3

Calculate the numerator for sinθ\sin \theta: x1y2x2y1=(23)(3)(1)(2)=632x_1y_2 - x_2y_1 = (2\sqrt{3})(3) - (1)(2) = 6\sqrt{3} - 2

Now, calculate sinθ\sin \theta: sinθ=63213\sin \theta = \frac{6\sqrt{3} - 2}{13} Since 636×1.732=10.3926\sqrt{3} \approx 6 \times 1.732 = 10.392, the numerator 6326\sqrt{3} - 2 is positive, so sinθ>0\sin \theta > 0. This is consistent with a counter-clockwise rotation.

Calculate tanθ\tan \theta: tanθ=sinθcosθ=6321343+313=63243+3\tan \theta = \frac{\sin \theta}{\cos \theta} = \frac{\frac{6\sqrt{3} - 2}{13}}{\frac{4\sqrt{3} + 3}{13}} = \frac{6\sqrt{3} - 2}{4\sqrt{3} + 3}

Step 4: Compare the derived tanθ\tan \theta with the given expression to find α\alpha.

We are given the expression for tanθ\tan \theta: tanθ=(α32)(43+3)\tan \theta = {{\left( {\alpha \sqrt 3 - 2} \right)} \over {\left( {4\sqrt 3 + 3} \right)}}

Equate our derived expression for tanθ\tan \theta with the given one: 63243+3=α3243+3\frac{6\sqrt{3} - 2}{4\sqrt{3} + 3} = \frac{\alpha\sqrt{3} - 2}{4\sqrt{3} + 3}

Since the denominators are the same and non-zero, the numerators must be equal: 632=α326\sqrt{3} - 2 = \alpha\sqrt{3} - 2

Add 2 to both sides: 63=α36\sqrt{3} = \alpha\sqrt{3}

Divide both sides by 3\sqrt{3}: α=6\alpha = 6


Common Mistakes & Tips

  • Forgetting the p>0p>0 constraint: This can lead to using the incorrect value of pp, resulting in an incorrect final answer. Always check problem constraints carefully.
  • Sign errors in sinθ\sin \theta: The direction of rotation (counter-clockwise) is crucial for determining the sign of sinθ\sin \theta. Using the cross product formula for sinθ\sin \theta is a reliable way to handle this.
  • Algebraic simplification errors: Be meticulous when simplifying expressions, especially nested radicals. Double-checking the factorization or quadratic formula application is recommended.

Summary

The problem required us to first find the value of pp by utilizing the property that vector rotation preserves magnitude. After determining p=2p=2, we explicitly defined the vectors and used the dot product to find cosθ\cos \theta. The direction of rotation provided the necessary information to determine the sign of sinθ\sin \theta. Finally, by calculating tanθ\tan \theta and equating it to the given expression, we solved for the unknown α\alpha.

The final answer is \boxed{6}.

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