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Part CCSIR NET June 2024the-jacobian-adds-a-power-of-r

The jacobian adds a power of r

Consider a solid torus of constant density ρ\rho, formed by revolving the disc (y−b)2+z2≤a2,x=0(y - b)^{2} + z^{2} \le a^{2}, x = 0 about the z-axis, where 0 < a < b. Then the moment of inertia of the solid torus about the z-axis is

  1. A.2π2a2b2(4b2+3a2)ρ2\pi^{2}a^{2}b^{2}(4b^{2} + 3a^{2})\rho
  2. B.(π2/2)a2b(4b2+3a2)ρ(\pi^{2}/2)a^{2}b(4b^{2} + 3a^{2})\rho✓ Correct
  3. C.(π2/2)a2b(4a2+3b2)ρ(\pi^{2}/2)a^{2}b(4a^{2} + 3b^{2})\rho
  4. D.2π2a2b2(4a2+3b2)ρ2\pi^{2}a^{2}b^{2}(4a^{2} + 3b^{2})\rho

You have the answer. Trap Analysis is why the other three were written.

Not a worked solution repeated four times — the specific reasoning error each wrong option was built to reward, and why this one tests execution slip.

See pricing

50 are analysed free — try those first.

The trap it tests

Execution slip

The idea was right. The computation was not.

Drill statements like this

Related counterexample: The generalised momentum ∂L/∂q̇ always equals mass × velocity

More on this topic

The chapter behind this: Lagrangian mechanics — free to read

From Classical Mechanics › Lagrangian formalism and generalised coordinates

Last revised . Found a mistake? Tell us — corrections are the fastest thing we act on.

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