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Vector Algebra question

2011 · Shift 1 · Q38
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  5. /2011 · Shift 1 · Q38

Vector Algebra question

2011 · Shift 1 · Q38

JEE AdvancedMathematicsVector AlgebraMCQ+4 / −1
Let a→=i^+j^+k^, b→=i^−j^+k^\overrightarrow a = \widehat i + \widehat j + \widehat k,\,\overrightarrow b = \widehat i - \widehat j + \widehat ka=i+j​+k,b=i−j​+k and c→=i^−j^−k^\overrightarrow c = \widehat i - \widehat j - \widehat kc=i−j​−k be three vectors. A vector v→\overrightarrow vv in the plane of a→\overrightarrow aa and b→,\overrightarrow b ,b, whose projection on c→\overrightarrow cc is 13{{1 \over {\sqrt 3 }}}3​1​ , is given by
  1. A
    i^−3j^+3k^\widehat i - 3\widehat j + 3\widehat ki−3j​+3k
  2. B
    −3i^−3j^−k^-3\widehat i - 3\widehat j - \widehat k−3i−3j​−k
  3. C
    3i^−j^+3k^3\widehat i - \widehat j + 3\widehat k3i−j​+3k
  4. D
    i^+3j^−3k^\widehat i + 3\widehat j - 3\widehat ki+3j​−3k
View written solutionFree

Correct answer: C

Step-by-step Derivations:

1. Express vector v in terms of a and b

The problem states that vector v→\overrightarrow vv lies in the plane of vectors a→\overrightarrow aa and b→\overrightarrow bb. This means v→\overrightarrow vv can be expressed as a linear combination of a→\overrightarrow aa and b→\overrightarrow bb. Let v→=λa→+μb→\overrightarrow v = \lambda \overrightarrow a + \mu \overrightarrow bv=λa+μb for some scalars λ\lambdaλ and μ\muμ.

Given: a→=i^+j^+k^\overrightarrow a = \widehat i + \widehat j + \widehat ka=i+j​+k b→=i^−j^+k^\overrightarrow b = \widehat i - \widehat j + \widehat kb=i−j​+k

Substituting these into the expression for v→\overrightarrow vv: v→=λ(i^+j^+k^)+μ(i^−j^+k^)\overrightarrow v = \lambda (\widehat i + \widehat j + \widehat k) + \mu (\widehat i - \widehat j + \widehat k)v=λ(i+j​+k)+μ(i−j​+k) v→=(λ+μ)i^+(λ−μ)j^+(λ+μ)k^\overrightarrow v = (\lambda + \mu)\widehat i + (\lambda - \mu)\widehat j + (\lambda + \mu)\widehat kv=(λ+μ)i+(λ−μ)j​+(λ+μ)k

2. Use the projection condition

The projection of a vector v→\overrightarrow vv onto a vector c→\overrightarrow cc is given by the formula: Projection=v→⋅c→∣c→∣Projection = \frac{\overrightarrow v \cdot \overrightarrow c}{|\overrightarrow c|}Projection=∣c∣v⋅c​ We are given that the projection of v→\overrightarrow vv on c→\overrightarrow cc is 13\frac{1}{\sqrt{3}}3​1​.

Given c→=i^−j^−k^\overrightarrow c = \widehat i - \widehat j - \widehat kc=i−j​−k, let's first calculate its magnitude ∣c→∣|\overrightarrow c|∣c∣: ∣c→∣=12+(−1)2+(−1)2=1+1+1=3|\overrightarrow c| = \sqrt{1^2 + (-1)^2 + (-1)^2} = \sqrt{1 + 1 + 1} = \sqrt{3}∣c∣=12+(−1)2+(−1)2​=1+1+1​=3​

Now, let's calculate the dot product v→⋅c→\overrightarrow v \cdot \overrightarrow cv⋅c: v→⋅c→=[(λ+μ)i^+(λ−μ)j^+(λ+μ)k^]⋅[i^−j^−k^]\overrightarrow v \cdot \overrightarrow c = [(\lambda + \mu)\widehat i + (\lambda - \mu)\widehat j + (\lambda + \mu)\widehat k] \cdot [\widehat i - \widehat j - \widehat k]v⋅c=[(λ+μ)i+(λ−μ)j​+(λ+μ)k]⋅[i−j​−k] v→⋅c→=(λ+μ)(1)+(λ−μ)(−1)+(λ+μ)(−1)\overrightarrow v \cdot \overrightarrow c = (\lambda + \mu)(1) + (\lambda - \mu)(-1) + (\lambda + \mu)(-1)v⋅c=(λ+μ)(1)+(λ−μ)(−1)+(λ+μ)(−1) v→⋅c→=(λ+μ)−(λ−μ)−(λ+μ)\overrightarrow v \cdot \overrightarrow c = (\lambda + \mu) - (\lambda - \mu) - (\lambda + \mu)v⋅c=(λ+μ)−(λ−μ)−(λ+μ) v→⋅c→=λ+μ−λ+μ−λ−μ=μ−λ\overrightarrow v \cdot \overrightarrow c = \lambda + \mu - \lambda + \mu - \lambda - \mu = \mu - \lambdav⋅c=λ+μ−λ+μ−λ−μ=μ−λ

Now we can use the projection equation: v→⋅c→∣c→∣=μ−λ3=13\frac{\overrightarrow v \cdot \overrightarrow c}{|\overrightarrow c|} = \frac{\mu - \lambda}{\sqrt{3}} = \frac{1}{\sqrt{3}}∣c∣v⋅c​=3​μ−λ​=3​1​ This implies μ−λ=1\mu - \lambda = 1μ−λ=1, or μ=λ+1\mu = \lambda + 1μ=λ+1.

3. Substitute to find the general form of v

Now we substitute μ=λ+1\mu = \lambda + 1μ=λ+1 back into our expression for v→\overrightarrow vv: v→=(λ+(λ+1))i^+(λ−(λ+1))j^+(λ+(λ+1))k^\overrightarrow v = (\lambda + (\lambda+1))\widehat i + (\lambda - (\lambda+1))\widehat j + (\lambda + (\lambda+1))\widehat kv=(λ+(λ+1))i+(λ−(λ+1))j​+(λ+(λ+1))k v→=(2λ+1)i^−1j^+(2λ+1)k^\overrightarrow v = (2\lambda + 1)\widehat i - 1\widehat j + (2\lambda + 1)\widehat kv=(2λ+1)i−1j​+(2λ+1)k

4. Match the general form with the given options

The general form of the vector v→\overrightarrow vv is (2λ+1)i^−j^+(2λ+1)k^(2\lambda + 1)\widehat i - \widehat j + (2\lambda + 1)\widehat k(2λ+1)i−j​+(2λ+1)k. We can see that the j^\widehat jj​ component of v→\overrightarrow vv must be −1-1−1. Let's check the options:

A: i^−3j^+3k^\widehat i - 3\widehat j + 3\widehat ki−3j​+3k (The j^\widehat jj​ component is -3. Incorrect.) B: −3i^−3j^−k^-3\widehat i - 3\widehat j - \widehat k−3i−3j​−k (The j^\widehat jj​ component is -3. Incorrect.) C: 3i^−j^+3k^3\widehat i - \widehat j + 3\widehat k3i−j​+3k (The j^\widehat jj​ component is -1. This is a possible answer.) D: i^+3j^−3k^\widehat i + 3\widehat j - 3\widehat ki+3j​−3k (The j^\widehat jj​ component is 3. Incorrect.)

Only option C has a j^\widehat jj​ component of −1-1−1. Let's verify if the other components match for some value of λ\lambdaλ. Comparing 3i^−j^+3k^3\widehat i - \widehat j + 3\widehat k3i−j​+3k with (2λ+1)i^−j^+(2λ+1)k^(2\lambda + 1)\widehat i - \widehat j + (2\lambda + 1)\widehat k(2λ+1)i−j​+(2λ+1)k, we must have: 2λ+1=32\lambda + 1 = 32λ+1=3 2λ=22\lambda = 22λ=2 λ=1\lambda = 1λ=1 This gives a consistent value for λ\lambdaλ. If λ=1\lambda=1λ=1, then μ=λ+1=2\mu = \lambda + 1 = 2μ=λ+1=2. The vector v→\overrightarrow vv is 1⋅a→+2⋅b→=(i^+j^+k^)+2(i^−j^+k^)=(1+2)i^+(1−2)j^+(1+2)k^=3i^−j^+3k^1 \cdot \overrightarrow a + 2 \cdot \overrightarrow b = (\widehat i + \widehat j + \widehat k) + 2(\widehat i - \widehat j + \widehat k) = (1+2)\widehat i + (1-2)\widehat j + (1+2)\widehat k = 3\widehat i - \widehat j + 3\widehat k1⋅a+2⋅b=(i+j​+k)+2(i−j​+k)=(1+2)i+(1−2)j​+(1+2)k=3i−j​+3k This matches option C perfectly.

Conclusion:

The vector v→\overrightarrow vv is 3i^−j^+3k^3\widehat i - \widehat j + 3\widehat k3i−j​+3k.

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