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JEE Main 2021
Vector Algebra
Vector Algebra
Medium

Question

Let a\overrightarrow a = 2i^\widehat i - 3j^\widehat j + 4k^\widehat k and b\overrightarrow b = 7i^\widehat i + j^\widehat j - 6k^\widehat k. If r\overrightarrow r ×\times a\overrightarrow a = r\overrightarrow r ×\times b\overrightarrow b , r\overrightarrow r . (i^\widehat i + 2j^\widehat j + k^\widehat k) = -3, then r\overrightarrow r . (2i^\widehat i - 3j^\widehat j + k^\widehat k) is equal to :

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Solution

Key Concepts and Formulas

  1. Vector Cross Product Property: For any vectors A\vec A, B\vec B, and C\vec C, A×B=A×C\vec A \times \vec B = \vec A \times \vec C implies A×(BC)=0\vec A \times (\vec B - \vec C) = \vec 0. This further implies that A\vec A is parallel to (BC)(\vec B - \vec C), meaning A=k(BC)\vec A = k(\vec B - \vec C) for some scalar kk.
  2. Scalar (Dot) Product: For vectors P=Pxi^+Pyj^+Pzk^\vec P = P_x\hat i + P_y\hat j + P_z\hat k and Q=Qxi^+Qyj^+Qzk^\vec Q = Q_x\hat i + Q_y\hat j + Q_z\hat k, their dot product is PQ=PxQx+PyQy+PzQz\vec P \cdot \vec Q = P_x Q_x + P_y Q_y + P_z Q_z.
  3. Vector Subtraction: To subtract vectors, subtract their corresponding components: (AxBx)i^+(AyBy)j^+(AzBz)k^(A_x - B_x)\hat i + (A_y - B_y)\hat j + (A_z - B_z)\hat k.

Step-by-Step Solution

Step 1: Simplify the first vector equation to determine the relationship between r\vec r and (ab)(\vec a - \vec b).

We are given the equation r×a=r×b\vec r \times \vec a = \vec r \times \vec b.

  • Why this step? This equation provides information about the orientation of r\vec r relative to a\vec a and b\vec b. We can simplify it using vector cross product properties.

Rearranging the terms, we get: r×ar×b=0\vec r \times \vec a - \vec r \times \vec b = \vec 0 Using the distributive property of the cross product, we have: r×(ab)=0\vec r \times (\vec a - \vec b) = \vec 0

  • Why this step? This simplified form tells us that r\vec r is parallel to the vector (ab)(\vec a - \vec b).

Now, let's calculate the vector (ab)(\vec a - \vec b): Given a=2i^3j^+4k^\vec a = 2\hat i - 3\hat j + 4\hat k and b=7i^+j^6k^\vec b = 7\hat i + \hat j - 6\hat k. ab=(27)i^+(31)j^+(4(6))k^\vec a - \vec b = (2 - 7)\hat i + (-3 - 1)\hat j + (4 - (-6))\hat k ab=5i^4j^+(4+6)k^\vec a - \vec b = -5\hat i - 4\hat j + (4 + 6)\hat k ab=5i^4j^+10k^\vec a - \vec b = -5\hat i - 4\hat j + 10\hat k Since r×(ab)=0\vec r \times (\vec a - \vec b) = \vec 0, r\vec r must be parallel to (ab)(\vec a - \vec b). Therefore, we can write r\vec r as a scalar multiple of (ab)(\vec a - \vec b): r=λ(ab)\vec r = \lambda (\vec a - \vec b) r=λ(5i^4j^+10k^)\vec r = \lambda (-5\hat i - 4\hat j + 10\hat k) where λ\lambda is a scalar constant.

Step 2: Use the second given condition to find the value of the scalar λ\lambda.

The second condition is r(i^+2j^+k^)=3\vec r \cdot (\hat i + 2\hat j + \hat k) = -3.

  • Why this step? We have an expression for r\vec r in terms of λ\lambda. Substituting this into the dot product equation will allow us to solve for the unknown scalar λ\lambda.

Substitute r=λ(5i^4j^+10k^)\vec r = \lambda (-5\hat i - 4\hat j + 10\hat k) into the equation: (λ(5i^4j^+10k^))(i^+2j^+k^)=3\left( \lambda (-5\hat i - 4\hat j + 10\hat k) \right) \cdot (\hat i + 2\hat j + \hat k) = -3 Factor out λ\lambda and compute the dot product: λ((5)(1)+(4)(2)+(10)(1))=3\lambda \left( (-5)(1) + (-4)(2) + (10)(1) \right) = -3 λ(58+10)=3\lambda \left( -5 - 8 + 10 \right) = -3 λ(13+10)=3\lambda \left( -13 + 10 \right) = -3 λ(3)=3\lambda (-3) = -3 Solving for λ\lambda: λ=33\lambda = \frac{-3}{-3} λ=1\lambda = 1

Step 3: Determine the vector r\vec r.

  • Why this step? Now that we have found the value of λ\lambda, we can determine the exact components of the vector r\vec r.

Substitute λ=1\lambda = 1 back into the expression for r\vec r from Step 1: r=1(5i^4j^+10k^)\vec r = 1 \cdot (-5\hat i - 4\hat j + 10\hat k) r=5i^4j^+10k^\vec r = -5\hat i - 4\hat j + 10\hat k

Step 4: Calculate the required dot product.

We need to find the value of r(2i^3j^+k^)\vec r \cdot (2\hat i - 3\hat j + \hat k).

  • Why this step? This is the final quantity we need to compute, and we now have the complete vector r\vec r.

Substitute the components of r\vec r and the target vector into the dot product: r(2i^3j^+k^)=(5i^4j^+10k^)(2i^3j^+k^)\vec r \cdot (2\hat i - 3\hat j + \hat k) = (-5\hat i - 4\hat j + 10\hat k) \cdot (2\hat i - 3\hat j + \hat k) Perform the dot product calculation: =(5)(2)+(4)(3)+(10)(1)= (-5)(2) + (-4)(-3) + (10)(1) =10+12+10= -10 + 12 + 10 =2+10= 2 + 10 =12= 12

Common Mistakes & Tips

  • Sign Errors: Pay close attention to signs during vector subtraction and dot product calculations. For example, 4(6)4 - (-6) is 4+64+6.
  • Cross Product Order: Remember that the cross product is not commutative (A×BB×A\vec A \times \vec B \neq \vec B \times \vec A). Ensure correct order when applying distributive properties.
  • Vector vs. Scalar: Differentiate between vector quantities (like r\vec r) and scalar quantities (like λ\lambda and the final dot product result).

Summary

The problem starts with a condition on the cross product of an unknown vector r\vec r with two given vectors a\vec a and b\vec b. This condition, r×a=r×b\vec r \times \vec a = \vec r \times \vec b, simplifies to r×(ab)=0\vec r \times (\vec a - \vec b) = \vec 0, implying that r\vec r is parallel to (ab)(\vec a - \vec b). We then express r\vec r as a scalar multiple, λ(ab)\lambda(\vec a - \vec b). The second condition, a dot product involving r\vec r, is used to solve for the scalar λ\lambda. Once λ\lambda is found, the vector r\vec r is determined, and the final required dot product can be calculated.

The final answer is 12\boxed{\text{12}}.

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