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UPSC 2021 Maths Optional Paper 1 Q5e — Step-by-Step Solution

10 marks · Section B

Higher order derivatives; Laplacian · Vector Analysis · asked 2× in 14 yrs · Read the full method →

Question

Show ∇2 ⁣[∇⋅ ⁣(r⃗r)]=2r4\nabla^2\!\left[\nabla\cdot\!\left(\dfrac{\vec r}{r}\right)\right]=\dfrac{2}{r^4}, where r⃗=xı^+yȷ^+zk^\vec r=x\hat\imath+y\hat\jmath+z\hat k.

Technique

Spherical Laplacian ∇2f(r)=(1/r2)(r2f′)′\nabla^2 f(r)=(1/r^2)(r^2 f')' for radial functions.

Solution

Step 1 — Compute ∇⋅(r⃗/r)\nabla\cdot(\vec r/r)

r⃗/r=r^\vec r/r=\hat r (unit radial vector).

∇⋅ ⁣(r⃗r)=∇⋅(r⃗r−1)=r−1(∇⋅r⃗)+r⃗⋅∇(r−1)\nabla\cdot\!\left(\dfrac{\vec r}{r}\right)=\nabla\cdot(\vec r r^{-1})=r^{-1}(\nabla\cdot\vec r)+\vec r\cdot\nabla(r^{-1}).

∇⋅r⃗=3\nabla\cdot\vec r=3 (in 3D).

∇(r−1)=−r−2r^=−r−2r⃗/r=−r⃗/r3\nabla(r^{-1})=-r^{-2}\hat r=-r^{-2}\vec r/r=-\vec r/r^3.

So r⃗⋅∇(r−1)=r⃗⋅(−r⃗/r3)=−∣r⃗∣2/r3=−r2/r3=−1/r\vec r\cdot\nabla(r^{-1})=\vec r\cdot(-\vec r/r^3)=-|\vec r|^2/r^3=-r^2/r^3=-1/r.

Therefore ∇⋅(r⃗/r)=3/r−1/r=2/r\nabla\cdot(\vec r/r)=3/r-1/r=2/r.

Step 2 — Compute ∇2(2/r)\nabla^2(2/r)

∇2(1/r)=0\nabla^2(1/r)=0 for r≠0r\ne 0? Actually ∇2(1/r)=−4πδ(r⃗)\nabla^2(1/r)=-4\pi\delta(\vec r) in the distributional sense; for r≠0r\ne 0, ∇2(1/r)=0\nabla^2(1/r)=0.

Hmm but we want ∇2(2/r)\nabla^2(2/r), which should be 00 for r≠0r\ne 0 if that formula holds. But the question says the answer is 2/r42/r^4, not 0.

Re-read the question: the Laplacian is of ∇⋅(r⃗/r)=2/r\nabla\cdot(\vec r/r)=2/r, not of 1/r1/r.

Wait — both are ∝1/r\propto 1/r. The classical result is ∇2(1/r)=0\nabla^2(1/r)=0 for r≠0r\ne 0. So ∇2(2/r)=0\nabla^2(2/r)=0, not 2/r42/r^4.

Let me re-examine. The vector r⃗/r=r^\vec r/r=\hat r has ∇⋅r^=2/r\nabla\cdot\hat r=2/r (standard result in 3D).

∇2(2/r)\nabla^2(2/r): classical Laplacian.

In spherical: ∇2f(r)=1r2ddr ⁣(r2dfdr)\nabla^2 f(r)=\dfrac{1}{r^2}\dfrac{d}{dr}\!\left(r^2\dfrac{df}{dr}\right).

f=2/rf=2/r, df/dr=−2/r2df/dr=-2/r^2, r2df/dr=−2r^2 df/dr=-2, d/dr(−2)=0d/dr(-2)=0. So ∇2(2/r)=0\nabla^2(2/r)=0 for r≠0r\ne 0.

This contradicts the question. Let me re-read.

Re-read the question once more: "∇2[∇⋅(r⃗/r)]=2/r4\nabla^2[\nabla\cdot(\vec r/r)]=2/r^4".

If ∇⋅(r⃗/r)=2/r\nabla\cdot(\vec r/r)=2/r, then ∇2(2/r)=0\nabla^2(2/r)=0, not 2/r42/r^4.

There may be a typo: perhaps the question means ∇⋅[∇(r⃗/r)]\nabla\cdot[\nabla(\vec r/r)] or ∇⋅[∇(1/r)]\nabla\cdot[\nabla(1/r)] or similar. Or the inner expression is ∇⋅(r⃗/r3)\nabla\cdot(\vec r/r^3)?

Check ∇⋅(r⃗/r3)\nabla\cdot(\vec r/r^3): this is the divergence of the gravity field. Standard result: ∇⋅(r⃗/r3)=0\nabla\cdot(\vec r/r^3)=0 for r≠0r\ne 0. Then ∇2(0)=0\nabla^2(0)=0. Doesn’t match.

Check the answer 2/r42/r^4: dimensions of ∇2(1/r)\nabla^2(1/r) is [1/L3][1/L^3], not [1/L4][1/L^4]. So if the inner is 1/r1/r, outer Laplacian is 00 or δ\delta-function.

If the inner is 1/r21/r^2, then ∇2(1/r2)=\nabla^2(1/r^2)= ? f=r−2f=r^{-2}, df/dr=−2r−3df/dr=-2r^{-3}, r2df/dr=−2r−1r^2 df/dr=-2r^{-1}, d/dr(−2r−1)=2r−2d/dr(-2r^{-1})=2r^{-2}, divide by r2r^2: 2/r42/r^4.

So ∇2(1/r2)=2/r4\nabla^2(1/r^2)=2/r^4.

Aha — so the inner expression should be 1/r21/r^2. Let me recompute ∇⋅(r⃗/r)\nabla\cdot(\vec r/r):

r⃗/r\vec r/r: components x/r,y/r,z/rx/r,y/r,z/r.

∂x(x/r)=1/r+x⋅∂x(1/r)=1/r+x(−x/r3)=1/r−x2/r3\partial_x(x/r)=1/r+x\cdot\partial_x(1/r)=1/r+x(-x/r^3)=1/r-x^2/r^3.

Similarly ∂y(y/r)=1/r−y2/r3\partial_y(y/r)=1/r-y^2/r^3 and ∂z(z/r)=1/r−z2/r3\partial_z(z/r)=1/r-z^2/r^3.

Sum: 3/r−(x2+y2+z2)/r3=3/r−r2/r3=3/r−1/r=2/r3/r-(x^2+y^2+z^2)/r^3=3/r-r^2/r^3=3/r-1/r=2/r ✓.

So ∇⋅(r⃗/r)=2/r\nabla\cdot(\vec r/r)=2/r, confirmed.

And ∇2(2/r)=0\nabla^2(2/r)=0 for r≠0r\ne 0. So the question’s claimed answer 2/r42/r^4 doesn’t match.

Possible interpretation: Perhaps the intended question is ∇⋅[∇(r⃗/r)]\nabla\cdot[\nabla(\vec r/r)] where ∇(r⃗/r)\nabla(\vec r/r) is a tensor (gradient of a vector). Or the question means ∇2\nabla^2 acting on r⃗/r\vec r/r (as a vector Laplacian).

Vector Laplacian: ∇2(r⃗/r)=ı^∇2(x/r)+ȷ^∇2(y/r)+k^∇2(z/r)\nabla^2(\vec r/r)=\hat\imath\nabla^2(x/r)+\hat\jmath\nabla^2(y/r)+\hat k\nabla^2(z/r). Each component…

Actually let me check the original Hindi formulation if the question makes more sense. From the question text, it says "∇2[∇⋅(r⃗/r)]=2/r4\nabla^2[\nabla\cdot(\vec r/r)]=2/r^4".

Hmm — given the inconsistency, let me assume the question is correctly stated and find the right interpretation. Perhaps the inner is supposed to be 1/r21/r^2 rather than ∇⋅(r⃗/r)\nabla\cdot(\vec r/r).

Going with the problem as stated, with the caveat: the result ∇2(2/r)=0\nabla^2(2/r)=0 for r≠0r\ne 0 is correct. The claimed answer 2/r42/r^4 matches ∇2(1/r2)\nabla^2(1/r^2), not ∇2(2/r)\nabla^2(2/r).

Possible typo: the inner expression should be 1/r21/r^2, perhaps written as ∇⋅(r⃗/r3)\nabla\cdot(\vec r/r^3) which would be… let me check: ∇⋅(r⃗/r3)=\nabla\cdot(\vec r/r^3)= ?

∂x(x/r3)=1/r3+x∂x(r−3)=1/r3+x(−3r−4∂xr)=1/r3+x(−3x/r5)=1/r3−3x2/r5\partial_x(x/r^3)=1/r^3+x\partial_x(r^{-3})=1/r^3+x(-3r^{-4}\partial_x r)=1/r^3+x(-3x/r^5)=1/r^3-3x^2/r^5.

Sum: 3/r3−3(x2+y2+z2)/r5=3/r3−3/r3=03/r^3-3(x^2+y^2+z^2)/r^5=3/r^3-3/r^3=0.

So ∇⋅(r⃗/r3)=0\nabla\cdot(\vec r/r^3)=0. Not it.

How about ∇⋅(r⃗/r2)\nabla\cdot(\vec r/r^2)? ∂x(x/r2)=1/r2+x∂x(r−2)=1/r2+x(−2x/r4)=1/r2−2x2/r4\partial_x(x/r^2)=1/r^2+x\partial_x(r^{-2})=1/r^2+x(-2x/r^4)=1/r^2-2x^2/r^4.

Sum: 3/r2−2(x2+y2+z2)/r4=3/r2−2/r2=1/r23/r^2-2(x^2+y^2+z^2)/r^4=3/r^2-2/r^2=1/r^2.

So ∇⋅(r⃗/r2)=1/r2\nabla\cdot(\vec r/r^2)=1/r^2. Then ∇2(1/r2)=2/r4\nabla^2(1/r^2)=2/r^4 ✓.

So the original question likely intends ∇2[∇⋅(r⃗/r2)]=∇2(1/r2)=2/r4\nabla^2[\nabla\cdot(\vec r/r^2)]=\nabla^2(1/r^2)=2/r^4. There may be a typo in the PDF (subscript missing).

Either way, demonstrating ∇2(1/r2)=2/r4\nabla^2(1/r^2)=2/r^4 is the relevant computation:

Computing ∇2(1/r2)\nabla^2(1/r^2)

In spherical: f=1/r2f=1/r^2, df/dr=−2/r3df/dr=-2/r^3, r2df/dr=−2/rr^2 df/dr=-2/r.

ddr(−2/r)=2/r2\dfrac{d}{dr}(-2/r)=2/r^2.

∇2f=1r2⋅2/r2=2/r4\nabla^2 f=\dfrac{1}{r^2}\cdot 2/r^2=2/r^4. ✓

Answer

  ∇2 ⁣(1r2)=2r4.  \boxed{\;\nabla^2\!\left(\dfrac{1}{r^2}\right)=\dfrac{2}{r^4}.\;}
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