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Q.For two vectors a⃗\vec{a} and b⃗\vec{b}: Assertion (A): ∣a⃗×b⃗∣2+(a⃗⋅b⃗)2=∣a⃗∣2∣b⃗∣2|\vec{a} \times \vec{b}|^2 + (\vec{a} \cdot \vec{b})^2 = |\vec{a}|^2 |\vec{b}|^2 Reason (R): ∣a⃗×b⃗∣=(a⃗⋅b⃗)tan⁡θ|\vec{a} \times \vec{b}| = (\vec{a} \cdot \vec{b}) \tan \theta, (θ≠π2)\left(\theta \neq \frac{\pi}{2}\right) (A) Both Assertion (A) and Reason (R) are true and the Reason (R) is the correct explanation of the Assertion (A). (B) Both Assertion (A) and Reason (R) are true, but Reason (R) is not the correct explanation of the Assertion (A). (C) Assertion (A) is true, but Reason (R) is false. (D) Assertion (A) is false, but Reason (R) is true.

CBSECBSE Class XII Board 2026MCQ· 1mImportance★★★★★
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Assertion (A) is a fundamental identity relating the magnitudes of the cross product and dot product, which is true. Reason (R) is also a true relationship between the magnitudes of the cross product and dot product, but it does not explain Assertion (A). The correct option is (B).

To evaluate this assertion-reason question, we need to understand the definitions of the dot product and cross product of two vectors and the geometric meaning of the angle between them. Both the dot product and the cross product are fundamental operations in vector algebra, and their properties are frequently tested.

The dot product (or scalar product) of two vectors a⃗\vec{a} and b⃗\vec{b} is defined as:

a⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡θ\vec{a} \cdot \vec{b} = |\vec{a}| |\vec{b}| \cos \theta

where ∣a⃗∣|\vec{a}| and ∣b⃗∣|\vec{b}| are the magnitudes of vectors a⃗\vec{a} and b⃗\vec{b} respectively, and θ\theta is the angle between them (0≤θ≤π0 \le \theta \le \pi). The result is a scalar.

The cross product (or vector product) of two vectors a⃗\vec{a} and b⃗\vec{b} results in a vector perpendicular to both a⃗\vec{a} and b⃗\vec{b}. Its magnitude is defined as:

∣a⃗×b⃗∣=∣a⃗∣∣b⃗∣sin⁡θ|\vec{a} \times \vec{b}| = |\vec{a}| |\vec{b}| \sin \theta

where θ\theta is again the angle between a⃗\vec{a} and b⃗\vec{b}. The direction of a⃗×b⃗\vec{a} \times \vec{b} is given by the right-hand rule.

Now, let's evaluate the Assertion and Reason.

  1. Evaluate Assertion (A):

    The assertion states: ∣a⃗×b⃗∣2+(a⃗⋅b⃗)2=∣a⃗∣2∣b⃗∣2|\vec{a} \times \vec{b}|^2 + (\vec{a} \cdot \vec{b})^2 = |\vec{a}|^2 |\vec{b}|^2.

    Let's substitute the definitions of ∣a⃗×b⃗∣|\vec{a} \times \vec{b}| and (a⃗⋅b⃗)(\vec{a} \cdot \vec{b}) into the left-hand side (LHS) of the equation.

    LHS =(∣a⃗∣∣b⃗∣sin⁡θ)2+(∣a⃗∣∣b⃗∣cos⁡θ)2= (|\vec{a}| |\vec{b}| \sin \theta)^2 + (|\vec{a}| |\vec{b}| \cos \theta)^2

    LHS =∣a⃗∣2∣b⃗∣2sin⁡2θ+∣a⃗∣2∣b⃗∣2cos⁡2θ= |\vec{a}|^2 |\vec{b}|^2 \sin^2 \theta + |\vec{a}|^2 |\vec{b}|^2 \cos^2 \theta

    We can factor out ∣a⃗∣2∣b⃗∣2|\vec{a}|^2 |\vec{b}|^2:

    LHS =∣a⃗∣2∣b⃗∣2(sin⁡2θ+cos⁡2θ)= |\vec{a}|^2 |\vec{b}|^2 (\sin^2 \theta + \cos^2 \theta)

    Important

    Recall the fundamental trigonometric identity: sin⁡2θ+cos⁡2θ=1\sin^2 \theta + \cos^2 \theta = 1.

    Using this identity:

    LHS =∣a⃗∣2∣b⃗∣2(1)= |\vec{a}|^2 |\vec{b}|^2 (1)

    LHS =∣a⃗∣2∣b⃗∣2= |\vec{a}|^2 |\vec{b}|^2

    This matches the right-hand side (RHS) of the assertion.

    Therefore, Assertion (A) is True. This identity is often known as Lagrange's Identity for vectors.

  2. Evaluate Reason (R):

    The reason states: ∣a⃗×b⃗∣=(a⃗⋅b⃗)tan⁡θ|\vec{a} \times \vec{b}| = (\vec{a} \cdot \vec{b}) \tan \theta, (θ≠π2)\left(\theta \neq \frac{\pi}{2}\right).

    Let's substitute the definitions of ∣a⃗×b⃗∣|\vec{a} \times \vec{b}| and (a⃗⋅b⃗)(\vec{a} \cdot \vec{b}) into this equation.

    LHS: ∣a⃗×b⃗∣=∣a⃗∣∣b⃗∣sin⁡θ|\vec{a} \times \vec{b}| = |\vec{a}| |\vec{b}| \sin \theta

    RHS: (a⃗⋅b⃗)tan⁡θ=(∣a⃗∣∣b⃗∣cos⁡θ)tan⁡θ(\vec{a} \cdot \vec{b}) \tan \theta = (|\vec{a}| |\vec{b}| \cos \theta) \tan \theta

    Recall the definition of tan⁡θ\tan \theta: tan⁡θ=sin⁡θcos⁡θ\tan \theta = \frac{\sin \theta}{\cos \theta}.

    Substitute this into the RHS:

    RHS =(∣a⃗∣∣b⃗∣cos⁡θ)(sin⁡θcos⁡θ)= (|\vec{a}| |\vec{b}| \cos \theta) \left(\frac{\sin \theta}{\cos \theta}\right)

    Since θ≠π2\theta \neq \frac{\pi}{2}, cos⁡θ≠0\cos \theta \neq 0, so we can cancel cos⁡θ\cos \theta: …

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