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Volume of Parallelepiped Formed by Vectors on Distance Constraint Plane

Let PP be the plane 3x+2y+3z=16\sqrt{3}x + 2y + 3z = 16 and let S={αi^+βj^+γk^:α2+β2+γ2=1 and the distance of (α,β,γ) from the plane P is 72}S = \left\{ \alpha \hat{i} + \beta \hat{j} + \gamma \hat{k} : \alpha^2 + \beta^2 + \gamma^2 = 1 \text{ and the distance of } (\alpha, \beta, \gamma) \text{ from the plane } P \text{ is } \frac{7}{2} \right\}. Let u,v\vec{u}, \vec{v} and w\vec{w} be three distinct vectors in SS such that uv=vw=wu|\vec{u} - \vec{v}| = |\vec{v} - \vec{w}| = |\vec{w} - \vec{u}|. Let VV be the volume of the parallelepiped determined by vectors u,v\vec{u}, \vec{v} and w\vec{w}. Then the value of 803V\frac{80}{\sqrt{3}}V is

Official Numerical Answer45

Step-by-Step Solution

To find the value of 803V\frac{80}{\sqrt{3}} V, we first analyze the set SS of vectors r=αi^+βj^+γk^\vec{r} = \alpha \hat{i} + \beta \hat{j} + \gamma \hat{k}.

Step 1: Geometry of the Set SS

The vectors in SS are unit vectors, which means their terminal points lie on the unit sphere: α2+β2+γ2=1    r=1\alpha^2 + \beta^2 + \gamma^2 = 1 \implies |\vec{r}| = 1

The distance dd of a point (α,β,γ)(\alpha, \beta, \gamma) from the plane P:3x+2y+3z=16P: \sqrt{3}x + 2y + 3z = 16 is given as 72\frac{7}{2}. Using the perpendicular distance formula: d=3α+2β+3γ16(3)2+22+32=3α+2β+3γ164=72d = \frac{|\sqrt{3}\alpha + 2\beta + 3\gamma - 16|}{\sqrt{(\sqrt{3})^2 + 2^2 + 3^2}} = \frac{|\sqrt{3}\alpha + 2\beta + 3\gamma - 16|}{4} = \frac{7}{2}

This yields: 3α+2β+3γ16=14|\sqrt{3}\alpha + 2\beta + 3\gamma - 16| = 14

So, we have two possible cases:

  1. 3α+2β+3γ=30\sqrt{3}\alpha + 2\beta + 3\gamma = 30
  2. 3α+2β+3γ=2\sqrt{3}\alpha + 2\beta + 3\gamma = 2

By the Cauchy-Schwarz Inequality, for any point on the unit sphere α2+β2+γ2=1\alpha^2 + \beta^2 + \gamma^2 = 1: 3α+2β+3γ(3)2+22+32α2+β2+γ2=41=4|\sqrt{3}\alpha + 2\beta + 3\gamma| \le \sqrt{(\sqrt{3})^2 + 2^2 + 3^2} \sqrt{\alpha^2 + \beta^2 + \gamma^2} = 4 \cdot 1 = 4

Hence, 3α+2β+3γ=30\sqrt{3}\alpha + 2\beta + 3\gamma = 30 is not possible. Therefore, we must have: 3α+2β+3γ=2\sqrt{3}\alpha + 2\beta + 3\gamma = 2

If we define the unit normal to the plane PP as n^=3i^+2j^+3k^4\hat{n} = \frac{\sqrt{3}\hat{i} + 2\hat{j} + 3\hat{k}}{4}, the condition becomes: rn^=24=12\vec{r} \cdot \hat{n} = \frac{2}{4} = \frac{1}{2}

Thus, the set SS represents a circle CC formed by the intersection of the unit sphere r=1|\vec{r}| = 1 and the plane rn^=12\vec{r} \cdot \hat{n} = \frac{1}{2}.

Step 2: Radius of Circle CC and Distance between Vectors

The distance from the origin to the plane of the circle CC is h=12h = \frac{1}{2}. The radius RR of the circle CC is: R=12h2=1(12)2=32R = \sqrt{1^2 - h^2} = \sqrt{1 - \left(\frac{1}{2}\right)^2} = \frac{\sqrt{3}}{2}

The vectors u,v,wS\vec{u}, \vec{v}, \vec{w} \in S form an equilateral triangle inscribed in this circle CC, as their mutual distances are equal: uv=vw=wu=a|\vec{u} - \vec{v}| = |\vec{v} - \vec{w}| = |\vec{w} - \vec{u}| = a

The side length aa of an equilateral triangle inscribed in a circle of radius RR is: a=R3=32×3=32a = R\sqrt{3} = \frac{\sqrt{3}}{2} \times \sqrt{3} = \frac{3}{2}

Step 3: Determining the Scalar Triple Product (Volume VV)

To find the volume V=[uvw]V = |[\vec{u} \quad \vec{v} \quad \vec{w}]| of the parallelepiped, we use the Gram determinant.

First, we find the dot products between the vectors: Since u=v=w=1|\vec{u}| = |\vec{v}| = |\vec{w}| = 1: uv2=u2+v22(uv)=(32)2|\vec{u} - \vec{v}|^2 = |\vec{u}|^2 + |\vec{v}|^2 - 2(\vec{u} \cdot \vec{v}) = \left(\frac{3}{2}\right)^2 1+12(uv)=94    2(uv)=14    uv=181 + 1 - 2(\vec{u} \cdot \vec{v}) = \frac{9}{4} \implies 2(\vec{u} \cdot \vec{v}) = -\frac{1}{4} \implies \vec{u} \cdot \vec{v} = -\frac{1}{8}

By symmetry: uv=vw=wu=18\vec{u} \cdot \vec{v} = \vec{v} \cdot \vec{w} = \vec{w} \cdot \vec{u} = -\frac{1}{8}

The square of the scalar triple product is given by the determinant of the Gram matrix: V2=[uvw]2=uuuvuwvuvvvwwuwvww=11/81/81/811/81/81/81V^2 = [\vec{u} \quad \vec{v} \quad \vec{w}]^2 = \begin{vmatrix} \vec{u} \cdot \vec{u} & \vec{u} \cdot \vec{v} & \vec{u} \cdot \vec{w} \\ \vec{v} \cdot \vec{u} & \vec{v} \cdot \vec{v} & \vec{v} \cdot \vec{w} \\ \vec{w} \cdot \vec{u} & \vec{w} \cdot \vec{v} & \vec{w} \cdot \vec{w} \end{vmatrix} = \begin{vmatrix} 1 & -1/8 & -1/8 \\ -1/8 & 1 & -1/8 \\ -1/8 & -1/8 & 1 \end{vmatrix}

Evaluating the determinant: V2=1(1164)(18)(18164)+(18)(164(18))V^2 = 1\left(1 - \frac{1}{64}\right) - \left(-\frac{1}{8}\right)\left(-\frac{1}{8} - \frac{1}{64}\right) + \left(-\frac{1}{8}\right)\left(\frac{1}{64} - \left(-\frac{1}{8}\right)\right) V2=636495129512=636418512=50418512=486512=243256V^2 = \frac{63}{64} - \frac{9}{512} - \frac{9}{512} = \frac{63}{64} - \frac{18}{512} = \frac{504 - 18}{512} = \frac{486}{512} = \frac{243}{256}

Taking the square root to find VV: V=243256=9316V = \sqrt{\frac{243}{256}} = \frac{9\sqrt{3}}{16}

Step 4: Final Calculation

We need to calculate 803V\frac{80}{\sqrt{3}}V: 803V=803×9316=5×9=45\frac{80}{\sqrt{3}} V = \frac{80}{\sqrt{3}} \times \frac{9\sqrt{3}}{16} = 5 \times 9 = 45