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Coplanarity and Parallelism Conditions on Unit Vectors

If a⃗,b⃗,c⃗\vec{a}, \vec{b}, \vec{c} and d⃗\vec{d} are unit vectors such that
(a⃗×b⃗)⋅(c⃗×d⃗)=1(\vec{a} \times \vec{b}) \cdot (\vec{c} \times \vec{d}) = 1
and a⃗⋅c⃗=12\vec{a} \cdot \vec{c} = \frac{1}{2},
then

Options

A

a⃗,b⃗,c⃗\vec{a}, \vec{b}, \vec{c} are non-coplanar

B

b⃗,c⃗,d⃗\vec{b}, \vec{c}, \vec{d} are non-coplanar

C

b⃗,d⃗\vec{b}, \vec{d} are non-parallel

Correct
D

a⃗,d⃗\vec{a}, \vec{d} are parallel and b⃗,c⃗\vec{b}, \vec{c} are parallel

Step-by-Step Solution

To determine the correct option, let us analyze the given conditions step-by-step:

  1. Magnitudes of Cross Products:
    We are given that a⃗,b⃗,c⃗,\vec{a}, \vec{b}, \vec{c}, and d⃗\vec{d} are unit vectors, so:
    ∣a⃗∣=∣b⃗∣=∣c⃗∣=∣d⃗∣=1|\vec{a}| = |\vec{b}| = |\vec{c}| = |\vec{d}| = 1
    The magnitude of the cross product of two unit vectors satisfies:
    ∣a⃗×b⃗∣=∣a⃗∣∣b⃗∣sin⁡θ1=sin⁡θ1≤1|\vec{a} \times \vec{b}| = |\vec{a}||\vec{b}|\sin\theta_1 = \sin\theta_1 \le 1
    ∣c⃗×d⃗∣=∣c⃗∣∣d⃗∣sin⁡θ2=sin⁡θ2≤1|\vec{c} \times \vec{d}| = |\vec{c}||\vec{d}|\sin\theta_2 = \sin\theta_2 \le 1
    where θ1\theta_1 is the angle between a⃗\vec{a} and b⃗\vec{b}, and θ2\theta_2 is the angle between c⃗\vec{c} and d⃗\vec{d}.

  2. Analysis of the Dot Product Equality:
    We are given:
    (a⃗×b⃗)⋅(c⃗×d⃗)=1(\vec{a} \times \vec{b}) \cdot (\vec{c} \times \vec{d}) = 1
    By the Cauchy-Schwarz inequality for the dot product:
    (a⃗×b⃗)⋅(c⃗×d⃗)≤∣a⃗×b⃗∣∣c⃗×d⃗∣≤1⋅1=1(\vec{a} \times \vec{b}) \cdot (\vec{c} \times \vec{d}) \le |\vec{a} \times \vec{b}| |\vec{c} \times \vec{d}| \le 1 \cdot 1 = 1
    For the dot product to achieve its maximum possible value of 11, the following must hold simultaneously:

    • ∣a⃗×b⃗∣=1  ⟹  a⃗⊥b⃗|\vec{a} \times \vec{b}| = 1 \implies \vec{a} \perp \vec{b}
    • ∣c⃗×d⃗∣=1  ⟹  c⃗⊥d⃗|\vec{c} \times \vec{d}| = 1 \implies \vec{c} \perp \vec{d}
    • The vectors a⃗×b⃗\vec{a} \times \vec{b} and c⃗×d⃗\vec{c} \times \vec{d} are in the same direction, meaning:
      a⃗×b⃗=c⃗×d⃗=n^\vec{a} \times \vec{b} = \vec{c} \times \vec{d} = \hat{n}
      where n^\hat{n} is a common unit normal vector.
  3. Coplanarity of the Vectors:
    Since a⃗×b⃗=n^\vec{a} \times \vec{b} = \hat{n} and c⃗×d⃗=n^\vec{c} \times \vec{d} = \hat{n}, all four vectors a⃗,b⃗,c⃗,\vec{a}, \vec{b}, \vec{c}, and d⃗\vec{d} are orthogonal to the same unit vector n^\hat{n}. Consequently, all four vectors lie in the same plane perpendicular to n^\hat{n}.

    • Thus, any set of three vectors among them, such as {a⃗,b⃗,c⃗}\{\vec{a}, \vec{b}, \vec{c}\} and {b⃗,c⃗,d⃗}\{\vec{b}, \vec{c}, \vec{d}\}, are coplanar.
    • This rules out options (A) and (B).
  4. Relationship Between b⃗\vec{b} and d⃗\vec{d}:
    Using the Lagrange's identity for the scalar product of cross products:
    (a⃗×b⃗)⋅(c⃗×d⃗)=(a⃗⋅c⃗)(b⃗⋅d⃗)−(a⃗⋅d⃗)(b⃗⋅c⃗)(\vec{a} \times \vec{b}) \cdot (\vec{c} \times \vec{d}) = (\vec{a} \cdot \vec{c})(\vec{b} \cdot \vec{d}) - (\vec{a} \cdot \vec{d})(\vec{b} \cdot \vec{c})
    Alternatively, since all vectors lie in the same plane:

    • b⃗\vec{b} is obtained by rotating a⃗\vec{a} by an angle of +90∘+90^\circ in the plane.
    • d⃗\vec{d} is obtained by rotating c⃗\vec{c} by the same angle of +90∘+90^\circ in the plane.

    The angle between b⃗\vec{b} and d⃗\vec{d} is therefore identical to the angle between a⃗\vec{a} and c⃗\vec{c}. Hence:
    b⃗⋅d⃗=a⃗⋅c⃗=12\vec{b} \cdot \vec{d} = \vec{a} \cdot \vec{c} = \frac{1}{2}

  5. Parallelism Condition:
    For unit vectors b⃗\vec{b} and d⃗\vec{d} to be parallel, their dot product must be ±1\pm 1:
    b⃗⋅d⃗=±1\vec{b} \cdot \vec{d} = \pm 1
    Since b⃗⋅d⃗=12≠±1\vec{b} \cdot \vec{d} = \frac{1}{2} \ne \pm 1, the vectors b⃗\vec{b} and d⃗\vec{d} are non-parallel.

    • Similarly, since a⃗⋅c⃗=12\vec{a} \cdot \vec{c} = \frac{1}{2}, a⃗\vec{a} and c⃗\vec{c} are non-parallel, which also implies a⃗\vec{a} and d⃗\vec{d} cannot be parallel as c⃗⊥d⃗\vec{c} \perp \vec{d}. This rules out option (D).

Therefore, b⃗\vec{b} and d⃗\vec{d} are non-parallel.

Correct Answer: C