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If a⃗=i^+k^\vec{a} = \hat{i} + \hat{k}, b⃗=j^−k^\vec{b} = \hat{j} - \hat{k} and c⃗=i^+j^+k^\vec{c} = \hat{i} + \hat{j} + \hat{k} 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 r⃗\vec{r} is:

Solution

✅ Correct Option: 1

Given three vectors:

a⃗=i^+k^\vec{a} = \hat{i} + \hat{k}

b⃗=j^−k^\vec{b} = \hat{j} - \hat{k}

c⃗=i^+j^+k^\vec{c} = \hat{i} + \hat{j} + \hat{k}

And two conditions about the unknown vector r⃗\vec{r}:

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

r⃗⋅a⃗=0\vec{r} \cdot \vec{a} = 0


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

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

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

When the cross product of two vectors equals zero, those vectors are parallel to each other.

So r⃗−c⃗\vec{r} - \vec{c} is parallel to b⃗\vec{b}.

This means:

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

where λ\lambda is some scalar.

Therefore:

r⃗=c⃗+λb⃗\vec{r} = \vec{c} + \lambda \vec{b}


Substituting the known vectors:

r⃗=(i^+j^+k^)+λ(j^−k^)\vec{r} = (\hat{i} + \hat{j} + \hat{k}) + \lambda(\hat{j} - \hat{k})

r⃗=i^+j^+k^+λj^−λk^\vec{r} = \hat{i} + \hat{j} + \hat{k} + \lambda\hat{j} - \lambda\hat{k}

r⃗=i^+(1+λ)j^+(1−λ)k^\vec{r} = \hat{i} + (1+\lambda)\hat{j} + (1-\lambda)\hat{k}


Using the condition r⃗⋅a⃗=0\vec{r} \cdot \vec{a} = 0:

[i^+(1+λ)j^+(1−λ)k^]⋅[i^+k^]=0[\hat{i} + (1+\lambda)\hat{j} + (1-\lambda)\hat{k}] \cdot [\hat{i} + \hat{k}] = 0

(1)(1)+(1+λ)(0)+(1−λ)(1)=0(1)(1) + (1+\lambda)(0) + (1-\lambda)(1) = 0

1+0+1−λ=01 + 0 + 1 - \lambda = 0

2−λ=02 - \lambda = 0

λ=2\lambda = 2


Substituting λ=2\lambda = 2:

r⃗=i^+(1+2)j^+(1−2)k^\vec{r} = \hat{i} + (1+2)\hat{j} + (1-2)\hat{k}

r⃗=i^+3j^−k^\vec{r} = \hat{i} + 3\hat{j} - \hat{k}

Therefore, r⃗=i^+3j^−k^\vec{r} = \hat{i} + 3\hat{j} - \hat{k}

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