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Dot Product of Vector r and Vector b

Let a⃗=−i^−k^\vec{a} = -\hat{i} - \hat{k}, b⃗=−i^+j^\vec{b} = -\hat{i} + \hat{j} and c⃗=i^+2j^+3k^\vec{c} = \hat{i} + 2\hat{j} + 3\hat{k} be three given vectors. If r⃗\vec{r} is a vector such that r⃗×b⃗=c⃗×b⃗\vec{r} \times \vec{b} = \vec{c} \times \vec{b} and r⃗⋅a⃗=0\vec{r} \cdot \vec{a} = 0, then the value of r⃗⋅b⃗\vec{r} \cdot \vec{b} is

Official Numerical Answer9

Step-by-Step Solution

To find the value of r⃗⋅b⃗\vec{r} \cdot \vec{b}, we begin with the given vector equation:

r⃗×b⃗=c⃗×b⃗\vec{r} \times \vec{b} = \vec{c} \times \vec{b}

Rearranging the terms gives:

(r⃗−c⃗)×b⃗=0⃗(\vec{r} - \vec{c}) \times \vec{b} = \vec{0}

This implies that the vector (r⃗−c⃗)(\vec{r} - \vec{c}) is parallel to b⃗\vec{b}. Thus, there exists a scalar λ\lambda such that:

r⃗−c⃗=λb⃗  ⟹  r⃗=c⃗+λb⃗\vec{r} - \vec{c} = \lambda \vec{b} \implies \vec{r} = \vec{c} + \lambda \vec{b}

We are given the condition r⃗⋅a⃗=0\vec{r} \cdot \vec{a} = 0. Substituting r⃗=c⃗+λb⃗\vec{r} = \vec{c} + \lambda \vec{b} into this condition:

(c⃗+λb⃗)⋅a⃗=0(\vec{c} + \lambda \vec{b}) \cdot \vec{a} = 0
c⃗⋅a⃗+λ(b⃗⋅a⃗)=0\vec{c} \cdot \vec{a} + \lambda (\vec{b} \cdot \vec{a}) = 0

Now, using the given vectors:

  • a⃗=−i^−k^\vec{a} = -\hat{i} - \hat{k}
  • b⃗=−i^+j^\vec{b} = -\hat{i} + \hat{j}
  • c⃗=i^+2j^+3k^\vec{c} = \hat{i} + 2\hat{j} + 3\hat{k}

We calculate the dot products:

c⃗⋅a⃗=(i^+2j^+3k^)⋅(−i^−k^)=(1)(−1)+(2)(0)+(3)(−1)=−1−3=−4\vec{c} \cdot \vec{a} = (\hat{i} + 2\hat{j} + 3\hat{k}) \cdot (-\hat{i} - \hat{k}) = (1)(-1) + (2)(0) + (3)(-1) = -1 - 3 = -4

b⃗⋅a⃗=(−i^+j^)⋅(−i^−k^)=(−1)(−1)+(1)(0)+(0)(−1)=1\vec{b} \cdot \vec{a} = (-\hat{i} + \hat{j}) \cdot (-\hat{i} - \hat{k}) = (-1)(-1) + (1)(0) + (0)(-1) = 1

Substituting these values into the equation:

−4+λ(1)=0  ⟹  λ=4-4 + \lambda (1) = 0 \implies \lambda = 4

Now, we substitute λ=4\lambda = 4 into the expression for r⃗\vec{r}:

r⃗=c⃗+4b⃗\vec{r} = \vec{c} + 4\vec{b}

Finally, we compute r⃗⋅b⃗\vec{r} \cdot \vec{b}:

r⃗⋅b⃗=(c⃗+4b⃗)⋅b⃗=c⃗⋅b⃗+4∣b⃗∣2\vec{r} \cdot \vec{b} = (\vec{c} + 4\vec{b}) \cdot \vec{b} = \vec{c} \cdot \vec{b} + 4|\vec{b}|^2

Calculating c⃗⋅b⃗\vec{c} \cdot \vec{b} and ∣b⃗∣2|\vec{b}|^2:

c⃗⋅b⃗=(i^+2j^+3k^)⋅(−i^+j^)=(1)(−1)+(2)(1)+(3)(0)=1\vec{c} \cdot \vec{b} = (\hat{i} + 2\hat{j} + 3\hat{k}) \cdot (-\hat{i} + \hat{j}) = (1)(-1) + (2)(1) + (3)(0) = 1

∣b⃗∣2=(−1)2+(1)2+(0)2=2|\vec{b}|^2 = (-1)^2 + (1)^2 + (0)^2 = 2

Thus,

r⃗⋅b⃗=1+4(2)=1+8=9\vec{r} \cdot \vec{b} = 1 + 4(2) = 1 + 8 = 9