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Miscellaneous Exercise · Q11

Q.Show that the direction cosines of a vector equally inclined to the axes OX, OY and OZ are ±(13,13,13)\pm \left(\frac{1}{\sqrt{3}}, \frac{1}{\sqrt{3}}, \frac{1}{\sqrt{3}}\right).

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A vector equally inclined to all three coordinate axes must have direction cosines that are all equal in magnitude. Using the identity l2+m2+n2=1l^2 + m^2 + n^2 = 1, each direction cosine becomes ±13\pm \frac{1}{\sqrt{3}}, giving the required result.

The key idea is simple: if a vector makes the same angle with the x‑axis, y‑axis, and z‑axis, then its direction cosines — which are the cosines of those angles — must all be equal. Let’s call that common value kk.

Direction cosines are not independent; they always satisfy l2+m2+n2=1l^2 + m^2 + n^2 = 1, because they are the components of a unit vector along the given direction. So if l=m=n=kl = m = n = k, we get:

k2+k2+k2=1⇒3k2=1⇒k2=13⇒k=±13.k^2 + k^2 + k^2 = 1 \quad\Rightarrow\quad 3k^2 = 1 \quad\Rightarrow\quad k^2 = \frac{1}{3} \quad\Rightarrow\quad k = \pm \frac{1}{\sqrt{3}}.

That’s the entire derivation. But let’s walk through it carefully, step by step.

  1. Define direction cosines.

    For a vector r⃗\vec{r}, the direction cosines are l=cos⁡αl = \cos \alpha, m=cos⁡βm = \cos \beta, n=cos⁡γn = \cos \gamma, where α,β,γ\alpha, \beta, \gamma are the angles r⃗\vec{r} makes with OX, OY, OZ respectively.

  2. Apply the condition “equally inclined”.

    “Equally inclined” means α=β=γ\alpha = \beta = \gamma. Therefore cos⁡α=cos⁡β=cos⁡γ\cos \alpha = \cos \beta = \cos \gamma, so l=m=nl = m = n. Let this common value be kk.

  3. Use the fundamental identity.

    For any vector, l2+m2+n2=1l^2 + m^2 + n^2 = 1. Substituting l=m=n=kl = m = n = k gives 3k2=13k^2 = 1.

  4. Solve for kk.

    k2=13k^2 = \frac{1}{3}, so k=±13k = \pm \frac{1}{\sqrt{3}}.

  5. Write the direction cosines. …

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