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JEE Main 2023
Vector Algebra
Vector Algebra
Hard

Question

Let a=9i^13j^+25k^,b=3i^+7j^13k^\vec{a}=9 \hat{i}-13 \hat{j}+25 \hat{k}, \vec{b}=3 \hat{i}+7 \hat{j}-13 \hat{k} and c=17i^2j^+k^\vec{c}=17 \hat{i}-2 \hat{j}+\hat{k} be three given vectors. If r\vec{r} is a vector such that r×a=(b+c)×a\vec{r} \times \vec{a}=(\vec{b}+\vec{c}) \times \vec{a} and r(bc)=0\vec{r} \cdot(\vec{b}-\vec{c})=0, then 593r+67a2(593)2\frac{|593 \vec{r}+67 \vec{a}|^2}{(593)^2} is equal to __________.

Answer: 9

Solution

Key Concepts and Formulas

  1. Vector Cross Product Property: If X×Y=Z×Y\vec{X} \times \vec{Y} = \vec{Z} \times \vec{Y} and Y0\vec{Y} \neq \vec{0}, then (XZ)×Y=0(\vec{X} - \vec{Z}) \times \vec{Y} = \vec{0}. This implies that XZ\vec{X} - \vec{Z} is parallel to Y\vec{Y}, meaning XZ=λY\vec{X} - \vec{Z} = \lambda \vec{Y} for some scalar λ\lambda.
  2. Vector Dot Product Properties:
    • Distributive Property: A(B+C)=AB+AC\vec{A} \cdot (\vec{B} + \vec{C}) = \vec{A} \cdot \vec{B} + \vec{A} \cdot \vec{C}.
    • Geometric Property: (B+C)(BC)=B2C2(\vec{B} + \vec{C}) \cdot (\vec{B} - \vec{C}) = |\vec{B}|^2 - |\vec{C}|^2.
  3. Magnitude of a Vector: For a vector V=xi^+yj^+zk^\vec{V} = x\hat{i} + y\hat{j} + z\hat{k}, its squared magnitude is V2=x2+y2+z2=VV|\vec{V}|^2 = x^2 + y^2 + z^2 = \vec{V} \cdot \vec{V}.
  4. Scalar Multiplication of Magnitude: For a scalar kk and vector V\vec{V}, kV2=k2V2|k\vec{V}|^2 = k^2 |\vec{V}|^2.

Problem Statement

Given vectors a=9i^13j^+25k^\vec{a}=9 \hat{i}-13 \hat{j}+25 \hat{k}, b=3i^+7j^13k^\vec{b}=3 \hat{i}+7 \hat{j}-13 \hat{k}, and c=17i^2j^+k^\vec{c}=17 \hat{i}-2 \hat{j}+\hat{k}. Find the value of 593r+67a2(593)2\frac{|593 \vec{r}+67 \vec{a}|^2}{(593)^2}, where r\vec{r} satisfies:

  1. r×a=(b+c)×a\vec{r} \times \vec{a}=(\vec{b}+\vec{c}) \times \vec{a}
  2. r(bc)=0\vec{r} \cdot(\vec{b}-\vec{c})=0

Step-by-Step Solution

Step 1: Determine the form of vector r\vec{r} using the first condition. The first condition is r×a=(b+c)×a\vec{r} \times \vec{a}=(\vec{b}+\vec{c}) \times \vec{a}. Rearranging this equation, we get: r×a(b+c)×a=0\vec{r} \times \vec{a} - (\vec{b}+\vec{c}) \times \vec{a} = \vec{0} Using the distributive property of the cross product, we can factor out a\vec{a}: (r(b+c))×a=0(\vec{r} - (\vec{b}+\vec{c})) \times \vec{a} = \vec{0} Since a\vec{a} is a non-zero vector, this implies that the vector (r(b+c))(\vec{r} - (\vec{b}+\vec{c})) must be parallel to a\vec{a}. Therefore, we can express this relationship as: r(b+c)=λa\vec{r} - (\vec{b}+\vec{c}) = \lambda \vec{a} for some scalar λ\lambda. This gives us an expression for r\vec{r}: r=(b+c)+λa(1)\vec{r} = (\vec{b}+\vec{c}) + \lambda \vec{a} \quad \cdots (1)

Step 2: Use the second condition to find the scalar λ\lambda. The second condition is r(bc)=0\vec{r} \cdot(\vec{b}-\vec{c})=0. Substitute the expression for r\vec{r} from equation (1) into this condition: ((b+c)+λa)(bc)=0((\vec{b}+\vec{c}) + \lambda \vec{a}) \cdot (\vec{b}-\vec{c}) = 0 Apply the distributive property of the dot product: (b+c)(bc)+λ(a(bc))=0(\vec{b}+\vec{c}) \cdot (\vec{b}-\vec{c}) + \lambda (\vec{a} \cdot (\vec{b}-\vec{c})) = 0 Using the identity (X+Y)(XY)=X2Y2(\vec{X}+\vec{Y}) \cdot (\vec{X}-\vec{Y}) = |\vec{X}|^2 - |\vec{Y}|^2, the first term becomes: b2c2+λ(a(bc))=0(2)|\vec{b}|^2 - |\vec{c}|^2 + \lambda (\vec{a} \cdot (\vec{b}-\vec{c})) = 0 \quad \cdots (2) Now, we compute the necessary vector components and their magnitudes/dot products: a=9i^13j^+25k^\vec{a}=9 \hat{i}-13 \hat{j}+25 \hat{k} b=3i^+7j^13k^\vec{b}=3 \hat{i}+7 \hat{j}-13 \hat{k} c=17i^2j^+k^\vec{c}=17 \hat{i}-2 \hat{j}+\hat{k}

Calculate b2|\vec{b}|^2: b2=(3)2+(7)2+(13)2=9+49+169=227|\vec{b}|^2 = (3)^2 + (7)^2 + (-13)^2 = 9 + 49 + 169 = 227 Calculate c2|\vec{c}|^2: c2=(17)2+(2)2+(1)2=289+4+1=294|\vec{c}|^2 = (17)^2 + (-2)^2 + (1)^2 = 289 + 4 + 1 = 294 Calculate the difference of squares: b2c2=227294=67|\vec{b}|^2 - |\vec{c}|^2 = 227 - 294 = -67 Calculate the vector bc\vec{b}-\vec{c}: bc=(317)i^+(7(2))j^+(131)k^=14i^+9j^14k^\vec{b}-\vec{c} = (3-17)\hat{i} + (7-(-2))\hat{j} + (-13-1)\hat{k} = -14\hat{i} + 9\hat{j} - 14\hat{k} Calculate the dot product a(bc)\vec{a} \cdot (\vec{b}-\vec{c}): a(bc)=(9)(14)+(13)(9)+(25)(14)\vec{a} \cdot (\vec{b}-\vec{c}) = (9)(-14) + (-13)(9) + (25)(-14) =126117350=593= -126 - 117 - 350 = -593 Substitute these values back into equation (2): 67+λ(593)=0-67 + \lambda (-593) = 0 593λ=67-593 \lambda = 67 λ=67593\lambda = -\frac{67}{593}

Step 3: Evaluate the target expression 593r+67a2(593)2\frac{|593 \vec{r}+67 \vec{a}|^2}{(593)^2}. First, simplify the term 593r+67a593 \vec{r}+67 \vec{a} by substituting the expression for r\vec{r} from equation (1) and the value of λ\lambda: 593r+67a=593((b+c)+λa)+67a593 \vec{r}+67 \vec{a} = 593 ((\vec{b}+\vec{c}) + \lambda \vec{a}) + 67 \vec{a} =593(b+c)+593λa+67a= 593 (\vec{b}+\vec{c}) + 593 \lambda \vec{a} + 67 \vec{a} =593(b+c)+(593λ+67)a= 593 (\vec{b}+\vec{c}) + (593 \lambda + 67) \vec{a} Substitute λ=67593\lambda = -\frac{67}{593}: 593λ+67=593(67593)+67=67+67=0593 \lambda + 67 = 593 \left(-\frac{67}{593}\right) + 67 = -67 + 67 = 0 So, the term simplifies to: 593r+67a=593(b+c)+(0)a=593(b+c)593 \vec{r}+67 \vec{a} = 593 (\vec{b}+\vec{c}) + (0) \vec{a} = 593 (\vec{b}+\vec{c}) Now substitute this into the expression to be evaluated: 593r+67a2(593)2=593(b+c)2(593)2\frac{|593 \vec{r}+67 \vec{a}|^2}{(593)^2} = \frac{|593 (\vec{b}+\vec{c})|^2}{(593)^2} Using the property kV2=k2V2|k\vec{V}|^2 = k^2 |\vec{V}|^2: (593)2(b+c)2(593)2=(b+c)2\frac{(593)^2 |(\vec{b}+\vec{c})|^2}{(593)^2} = |(\vec{b}+\vec{c})|^2 Finally, calculate b+c\vec{b}+\vec{c} and its squared magnitude: b+c=(3+17)i^+(72)j^+(13+1)k^\vec{b}+\vec{c} = (3+17)\hat{i} + (7-2)\hat{j} + (-13+1)\hat{k} b+c=20i^+5j^12k^\vec{b}+\vec{c} = 20\hat{i} + 5\hat{j} - 12\hat{k} Calculate the magnitude squared: (b+c)2=(20)2+(5)2+(12)2=400+25+144=569|(\vec{b}+\vec{c})|^2 = (20)^2 + (5)^2 + (-12)^2 = 400 + 25 + 144 = 569


Common Mistakes & Tips

  • Cross Product Interpretation: Be precise with the implication of (XZ)×Y=0(\vec{X} - \vec{Z}) \times \vec{Y} = \vec{0}. It means XZ\vec{X} - \vec{Z} is parallel to Y\vec{Y}, not necessarily that XZ=0\vec{X} - \vec{Z} = \vec{0} or X=Z\vec{X} = \vec{Z}.
  • Algebraic Simplification: The problem is designed for the term (593λ+67)(593\lambda + 67) to become zero. Always look for such cancellations, which often indicate a correct path or a simplified solution.
  • Component-wise Operations: Ensure accuracy when performing vector addition, subtraction, and dot products. A single arithmetic error in components can lead to an incorrect final answer.

Summary

The problem is solved by first using the cross product condition to establish the general form of r\vec{r} as r=(b+c)+λa\vec{r} = (\vec{b}+\vec{c}) + \lambda \vec{a}. The dot product condition is then used to solve for the scalar λ\lambda, which involves calculating the magnitudes of b\vec{b} and c\vec{c}, and the dot product of a\vec{a} with (bc)(\vec{b}-\vec{c}). Finally, substituting the derived r\vec{r} and the value of λ\lambda into the target expression 593r+67a2(593)2\frac{|593 \vec{r}+67 \vec{a}|^2}{(593)^2} leads to a significant simplification, where the terms involving λ\lambda cancel out, leaving the result as (b+c)2|(\vec{b}+\vec{c})|^2. The calculation of this magnitude squared yields the final answer.

The final answer is 569\boxed{569}.

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