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JEE Main 2023
Vector Algebra
Vector Algebra
Medium

Question

Let a^\hat{a} and b^\hat{b} be two unit vectors such that the angle between them is π4\frac{\pi}{4}. If θ\theta is the angle between the vectors (a^+b^)(\hat{a}+\hat{b}) and (a^+2b^+2(a^×b^))(\hat{a}+2 \hat{b}+2(\hat{a} \times \hat{b})), then the value of 164cos2θ164 \,\cos ^{2} \theta is equal to :

Options

Solution

Key Concepts and Formulas

  • Dot Product of Vectors: For two vectors U\vec{U} and V\vec{V}, the dot product is defined as UV=UVcosθ\vec{U} \cdot \vec{V} = |\vec{U}| |\vec{V}| \cos \theta, where θ\theta is the angle between them. This can be rearranged to find the cosine of the angle: cosθ=UVUV\cos \theta = \frac{\vec{U} \cdot \vec{V}}{|\vec{U}||\vec{V}|}.
  • Properties of Unit Vectors: A unit vector has a magnitude of 1. If a^\hat{a} and b^\hat{b} are unit vectors, then a^=1|\hat{a}| = 1 and b^=1|\hat{b}| = 1.
  • Cross Product of Unit Vectors: For unit vectors a^\hat{a} and b^\hat{b} with an angle α\alpha between them, the magnitude of their cross product is a^×b^=a^b^sinα=sinα|\hat{a} \times \hat{b}| = |\hat{a}| |\hat{b}| \sin \alpha = \sin \alpha. The direction of a^×b^\hat{a} \times \hat{b} is perpendicular to both a^\hat{a} and b^\hat{b}.
  • Scalar Triple Product Property: (A×B)C=A(B×C)(\vec{A} \times \vec{B}) \cdot \vec{C} = \vec{A} \cdot (\vec{B} \times \vec{C}). Also, if C\vec{C} is perpendicular to both A\vec{A} and B\vec{B}, then AC=0\vec{A} \cdot \vec{C} = 0 and BC=0\vec{B} \cdot \vec{C} = 0.

Step-by-Step Solution

Step 1: Define the vectors and given information. We are given two unit vectors a^\hat{a} and b^\hat{b} such that the angle between them is π4\frac{\pi}{4}. This means a^=1|\hat{a}| = 1, b^=1|\hat{b}| = 1, and the angle between a^\hat{a} and b^\hat{b} is α=π4\alpha = \frac{\pi}{4}.

Step 2: Identify the two vectors for which we need to find the angle θ\theta. Let U=a^+b^\vec{U} = \hat{a} + \hat{b} and V=a^+2b^+2(a^×b^)\vec{V} = \hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b}). We need to find the angle θ\theta between U\vec{U} and V\vec{V}.

Step 3: Calculate the dot product UV\vec{U} \cdot \vec{V}. We expand the dot product: UV=(a^+b^)(a^+2b^+2(a^×b^))\vec{U} \cdot \vec{V} = (\hat{a} + \hat{b}) \cdot (\hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b})) UV=a^(a^+2b^+2(a^×b^))+b^(a^+2b^+2(a^×b^))\vec{U} \cdot \vec{V} = \hat{a} \cdot (\hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b})) + \hat{b} \cdot (\hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b})) UV=(a^a^)+2(a^b^)+2(a^(a^×b^))+(b^a^)+2(b^b^)+2(b^(a^×b^))\vec{U} \cdot \vec{V} = (\hat{a} \cdot \hat{a}) + 2(\hat{a} \cdot \hat{b}) + 2(\hat{a} \cdot (\hat{a} \times \hat{b})) + (\hat{b} \cdot \hat{a}) + 2(\hat{b} \cdot \hat{b}) + 2(\hat{b} \cdot (\hat{a} \times \hat{b})) We know that a^a^=a^2=12=1\hat{a} \cdot \hat{a} = |\hat{a}|^2 = 1^2 = 1, b^b^=b^2=12=1\hat{b} \cdot \hat{b} = |\hat{b}|^2 = 1^2 = 1, and a^b^=b^a^=a^b^cos(π4)=1122=22\hat{a} \cdot \hat{b} = \hat{b} \cdot \hat{a} = |\hat{a}||\hat{b}|\cos(\frac{\pi}{4}) = 1 \cdot 1 \cdot \frac{\sqrt{2}}{2} = \frac{\sqrt{2}}{2}. The term a^(a^×b^)\hat{a} \cdot (\hat{a} \times \hat{b}) represents the scalar triple product of a^\hat{a}, a^\hat{a}, and b^\hat{b}. Since two of the vectors are identical, the scalar triple product is zero. This is because a^×b^\hat{a} \times \hat{b} is perpendicular to a^\hat{a}, so their dot product is 0. Similarly, b^(a^×b^)\hat{b} \cdot (\hat{a} \times \hat{b}) is also zero because a^×b^\hat{a} \times \hat{b} is perpendicular to b^\hat{b}. Substituting these values: UV=1+2(22)+2(0)+22+2(1)+2(0)\vec{U} \cdot \vec{V} = 1 + 2\left(\frac{\sqrt{2}}{2}\right) + 2(0) + \frac{\sqrt{2}}{2} + 2(1) + 2(0) UV=1+2+22+2=3+322\vec{U} \cdot \vec{V} = 1 + \sqrt{2} + \frac{\sqrt{2}}{2} + 2 = 3 + \frac{3\sqrt{2}}{2}

Step 4: Calculate the magnitude of vector U\vec{U}. U=a^+b^|\vec{U}| = |\hat{a} + \hat{b}| We use the property X2=XX|\vec{X}|^2 = \vec{X} \cdot \vec{X}: U2=(a^+b^)(a^+b^)=a^a^+2(a^b^)+b^b^|\vec{U}|^2 = (\hat{a} + \hat{b}) \cdot (\hat{a} + \hat{b}) = \hat{a} \cdot \hat{a} + 2(\hat{a} \cdot \hat{b}) + \hat{b} \cdot \hat{b} U2=1+2(22)+1=2+2|\vec{U}|^2 = 1 + 2\left(\frac{\sqrt{2}}{2}\right) + 1 = 2 + \sqrt{2} So, U=2+2|\vec{U}| = \sqrt{2 + \sqrt{2}}

Step 5: Calculate the magnitude of vector V\vec{V}. V2=a^+2b^+2(a^×b^)2|\vec{V}|^2 = |\hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b})|^2 Let W=a^×b^\vec{W} = \hat{a} \times \hat{b}. Then V=a^+2b^+2W\vec{V} = \hat{a} + 2\hat{b} + 2\vec{W}. We know that W\vec{W} is perpendicular to both a^\hat{a} and b^\hat{b}. V2=(a^+2b^+2W)(a^+2b^+2W)|\vec{V}|^2 = (\hat{a} + 2\hat{b} + 2\vec{W}) \cdot (\hat{a} + 2\hat{b} + 2\vec{W}) V2=a^a^+a^2b^+a^2W+2b^a^+2b^2b^+2b^2W+2Wa^+2W2b^+2W2W|\vec{V}|^2 = \hat{a} \cdot \hat{a} + \hat{a} \cdot 2\hat{b} + \hat{a} \cdot 2\vec{W} + 2\hat{b} \cdot \hat{a} + 2\hat{b} \cdot 2\hat{b} + 2\hat{b} \cdot 2\vec{W} + 2\vec{W} \cdot \hat{a} + 2\vec{W} \cdot 2\hat{b} + 2\vec{W} \cdot 2\vec{W} V2=a^2+2(a^b^)+2(a^W)+2(b^a^)+4b^2+4(b^W)+2(Wa^)+4(Wb^)+4W2|\vec{V}|^2 = |\hat{a}|^2 + 2(\hat{a} \cdot \hat{b}) + 2(\hat{a} \cdot \vec{W}) + 2(\hat{b} \cdot \hat{a}) + 4|\hat{b}|^2 + 4(\hat{b} \cdot \vec{W}) + 2(\vec{W} \cdot \hat{a}) + 4(\vec{W} \cdot \hat{b}) + 4|\vec{W}|^2 Since W=a^×b^\vec{W} = \hat{a} \times \hat{b}, we have: a^W=0\hat{a} \cdot \vec{W} = 0 b^W=0\hat{b} \cdot \vec{W} = 0 Wa^=0\vec{W} \cdot \hat{a} = 0 Wb^=0\vec{W} \cdot \hat{b} = 0 Also, W=a^×b^=a^b^sin(π4)=1122=22|\vec{W}| = |\hat{a} \times \hat{b}| = |\hat{a}||\hat{b}|\sin(\frac{\pi}{4}) = 1 \cdot 1 \cdot \frac{\sqrt{2}}{2} = \frac{\sqrt{2}}{2}. So, W2=(22)2=24=12|\vec{W}|^2 = \left(\frac{\sqrt{2}}{2}\right)^2 = \frac{2}{4} = \frac{1}{2} Substituting the known values: V2=1+2(22)+0+2(22)+4(1)+0+0+0+4(12)|\vec{V}|^2 = 1 + 2\left(\frac{\sqrt{2}}{2}\right) + 0 + 2\left(\frac{\sqrt{2}}{2}\right) + 4(1) + 0 + 0 + 0 + 4\left(\frac{1}{2}\right) V2=1+2+2+4+2=7+22|\vec{V}|^2 = 1 + \sqrt{2} + \sqrt{2} + 4 + 2 = 7 + 2\sqrt{2} So, V=7+22|\vec{V}| = \sqrt{7 + 2\sqrt{2}}

Step 6: Calculate cosθ\cos \theta. cosθ=UVUV=3+3222+27+22\cos \theta = \frac{\vec{U} \cdot \vec{V}}{|\vec{U}||\vec{V}|} = \frac{3 + \frac{3\sqrt{2}}{2}}{\sqrt{2 + \sqrt{2}} \sqrt{7 + 2\sqrt{2}}} cosθ=6+322(2+2)(7+22)=3(2+2)214+42+72+4\cos \theta = \frac{\frac{6 + 3\sqrt{2}}{2}}{\sqrt{(2 + \sqrt{2})(7 + 2\sqrt{2})}} = \frac{3(2 + \sqrt{2})}{2\sqrt{14 + 4\sqrt{2} + 7\sqrt{2} + 4}} cosθ=3(2+2)218+112\cos \theta = \frac{3(2 + \sqrt{2})}{2\sqrt{18 + 11\sqrt{2}}} This approach seems to lead to a complicated expression. Let's re-examine the problem and potentially find a simplification or an alternative calculation for cos2θ\cos^2 \theta.

Alternative Approach for cos2θ\cos^2 \theta

We need to calculate 164cos2θ164 \cos^2 \theta. Let's focus on calculating cos2θ\cos^2 \theta directly. cos2θ=(UV)2U2V2\cos^2 \theta = \frac{(\vec{U} \cdot \vec{V})^2}{|\vec{U}|^2 |\vec{V}|^2} From Step 3, UV=3+322=6+322\vec{U} \cdot \vec{V} = 3 + \frac{3\sqrt{2}}{2} = \frac{6 + 3\sqrt{2}}{2} (UV)2=(6+322)2=36+362+184=54+3624=27+1822(\vec{U} \cdot \vec{V})^2 = \left(\frac{6 + 3\sqrt{2}}{2}\right)^2 = \frac{36 + 36\sqrt{2} + 18}{4} = \frac{54 + 36\sqrt{2}}{4} = \frac{27 + 18\sqrt{2}}{2} From Step 4, U2=2+2|\vec{U}|^2 = 2 + \sqrt{2} From Step 5, V2=7+22|\vec{V}|^2 = 7 + 2\sqrt{2} Now, multiply the denominators: U2V2=(2+2)(7+22)=14+42+72+4=18+112|\vec{U}|^2 |\vec{V}|^2 = (2 + \sqrt{2})(7 + 2\sqrt{2}) = 14 + 4\sqrt{2} + 7\sqrt{2} + 4 = 18 + 11\sqrt{2} So, cos2θ=27+182218+112=27+1822(18+112)=9(3+22)2(18+112)\cos^2 \theta = \frac{\frac{27 + 18\sqrt{2}}{2}}{18 + 11\sqrt{2}} = \frac{27 + 18\sqrt{2}}{2(18 + 11\sqrt{2})} = \frac{9(3 + 2\sqrt{2})}{2(18 + 11\sqrt{2})} This still looks complicated. Let's check the calculations.

Let's re-evaluate the dot product UV\vec{U} \cdot \vec{V} and magnitudes. U=a^+b^\vec{U} = \hat{a} + \hat{b} V=a^+2b^+2(a^×b^)\vec{V} = \hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b})

Dot product: UV=(a^+b^)(a^+2b^+2(a^×b^))\vec{U} \cdot \vec{V} = (\hat{a} + \hat{b}) \cdot (\hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b})) =a^a^+2a^b^+2a^(a^×b^)+b^a^+2b^b^+2b^(a^×b^)= \hat{a}\cdot\hat{a} + 2\hat{a}\cdot\hat{b} + 2\hat{a}\cdot(\hat{a} \times \hat{b}) + \hat{b}\cdot\hat{a} + 2\hat{b}\cdot\hat{b} + 2\hat{b}\cdot(\hat{a} \times \hat{b}) =1+2(22)+0+22+2(1)+0= 1 + 2(\frac{\sqrt{2}}{2}) + 0 + \frac{\sqrt{2}}{2} + 2(1) + 0 =1+2+22+2=3+322= 1 + \sqrt{2} + \frac{\sqrt{2}}{2} + 2 = 3 + \frac{3\sqrt{2}}{2}. This is correct.

Magnitude of U\vec{U}: U2=(a^+b^)(a^+b^)=a^2+2a^b^+b^2=1+2(22)+1=2+2|\vec{U}|^2 = (\hat{a} + \hat{b}) \cdot (\hat{a} + \hat{b}) = |\hat{a}|^2 + 2\hat{a}\cdot\hat{b} + |\hat{b}|^2 = 1 + 2(\frac{\sqrt{2}}{2}) + 1 = 2 + \sqrt{2}. This is correct.

Magnitude of V\vec{V}: Let W=a^×b^\vec{W} = \hat{a} \times \hat{b}. W=22|\vec{W}| = \frac{\sqrt{2}}{2}. V2=a^+2b^+2W2|\vec{V}|^2 = |\hat{a} + 2\hat{b} + 2\vec{W}|^2 =(a^+2b^+2W)(a^+2b^+2W)= (\hat{a} + 2\hat{b} + 2\vec{W}) \cdot (\hat{a} + 2\hat{b} + 2\vec{W}) =a^2+2b^2+2W2+2(a^2b^)+2(a^2W)+2(2b^2W)= |\hat{a}|^2 + |2\hat{b}|^2 + |2\vec{W}|^2 + 2(\hat{a} \cdot 2\hat{b}) + 2(\hat{a} \cdot 2\vec{W}) + 2(2\hat{b} \cdot 2\vec{W}) =1+4(1)+4(12)+4a^b^+4a^W+8b^W= 1 + 4(1) + 4(\frac{1}{2}) + 4\hat{a}\cdot\hat{b} + 4\hat{a}\cdot\vec{W} + 8\hat{b}\cdot\vec{W} =1+4+2+4(22)+0+0= 1 + 4 + 2 + 4(\frac{\sqrt{2}}{2}) + 0 + 0 =7+22= 7 + 2\sqrt{2}. This is also correct.

Now, let's calculate 164cos2θ164 \cos^2 \theta: 164cos2θ=164(UV)2U2V2164 \cos^2 \theta = 164 \frac{(\vec{U} \cdot \vec{V})^2}{|\vec{U}|^2 |\vec{V}|^2} 164cos2θ=164(3+322)2(2+2)(7+22)164 \cos^2 \theta = 164 \frac{\left(3 + \frac{3\sqrt{2}}{2}\right)^2}{(2 + \sqrt{2})(7 + 2\sqrt{2})} 164cos2θ=164(6+322)218+112164 \cos^2 \theta = 164 \frac{\left(\frac{6 + 3\sqrt{2}}{2}\right)^2}{18 + 11\sqrt{2}} 164cos2θ=16436+362+18418+112=16454+362418+112164 \cos^2 \theta = 164 \frac{\frac{36 + 36\sqrt{2} + 18}{4}}{18 + 11\sqrt{2}} = 164 \frac{\frac{54 + 36\sqrt{2}}{4}}{18 + 11\sqrt{2}} 164cos2θ=16454+3624(18+112)=4154+36218+112164 \cos^2 \theta = 164 \frac{54 + 36\sqrt{2}}{4(18 + 11\sqrt{2})} = 41 \frac{54 + 36\sqrt{2}}{18 + 11\sqrt{2}} 164cos2θ=4118(3+22)18+112164 \cos^2 \theta = 41 \frac{18(3 + 2\sqrt{2})}{18 + 11\sqrt{2}} Let's try to rationalize the denominator 18+11218 + 11\sqrt{2}. Multiply by the conjugate 1811218 - 11\sqrt{2}: 18(3+22)18+112×1811218112=18((3)(18)(3)(112)+(22)(18)(22)(112))182(112)2\frac{18(3 + 2\sqrt{2})}{18 + 11\sqrt{2}} \times \frac{18 - 11\sqrt{2}}{18 - 11\sqrt{2}} = \frac{18( (3)(18) - (3)(11\sqrt{2}) + (2\sqrt{2})(18) - (2\sqrt{2})(11\sqrt{2}) )}{18^2 - (11\sqrt{2})^2} =18(54332+36244)324121(2)=18(10+32)324242=18(10+32)82= \frac{18(54 - 33\sqrt{2} + 36\sqrt{2} - 44)}{324 - 121(2)} = \frac{18(10 + 3\sqrt{2})}{324 - 242} = \frac{18(10 + 3\sqrt{2})}{82} =9(10+32)41= \frac{9(10 + 3\sqrt{2})}{41} Now, substitute this back into the expression for 164cos2θ164 \cos^2 \theta: 164cos2θ=41×9(10+32)41=9(10+32)=90+272164 \cos^2 \theta = 41 \times \frac{9(10 + 3\sqrt{2})}{41} = 9(10 + 3\sqrt{2}) = 90 + 27\sqrt{2}

Step 7: Verify the result with the options. The calculated value is 90+27290 + 27\sqrt{2}. This matches option (A).

Common Mistakes & Tips

  • Scalar Triple Product: Remember that the scalar triple product of three vectors where two are identical (e.g., a(a×b)\vec{a} \cdot (\vec{a} \times \vec{b})) is always zero.
  • Magnitude Calculation: When calculating the square of the magnitude of a sum of vectors, expand it fully and use the properties of dot products. For example, a+b2=(a+b)(a+b)=a2+b2+2ab|\vec{a} + \vec{b}|^2 = (\vec{a} + \vec{b}) \cdot (\vec{a} + \vec{b}) = |\vec{a}|^2 + |\vec{b}|^2 + 2\vec{a} \cdot \vec{b}.
  • Cross Product of Unit Vectors: Be careful with the magnitude of the cross product of unit vectors: a^×b^=sinα|\hat{a} \times \hat{b}| = \sin \alpha, where α\alpha is the angle between them.

Summary

The problem required finding the angle θ\theta between two complex vectors U=a^+b^\vec{U} = \hat{a} + \hat{b} and V=a^+2b^+2(a^×b^)\vec{V} = \hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b}), given that a^\hat{a} and b^\hat{b} are unit vectors with an angle of π4\frac{\pi}{4} between them. We used the dot product formula cosθ=UVUV\cos \theta = \frac{\vec{U} \cdot \vec{V}}{|\vec{U}||\vec{V}|} and calculated cos2θ=(UV)2U2V2\cos^2 \theta = \frac{(\vec{U} \cdot \vec{V})^2}{|\vec{U}|^2 |\vec{V}|^2}. By carefully expanding the dot products and magnitudes, and utilizing the properties of unit vectors and the cross product, we found the value of 164cos2θ164 \cos^2 \theta to be 90+27290 + 27\sqrt{2}.

The final answer is \boxed{90+27 \sqrt{2}}.

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