What is the final form of the generalized inertia tensor matrix M in generalized coordinates?

The final form of the generalized inertia tensor matrix M\mathbf{M} is: M=(MrrMrφMφrMφφ)=(m1+m200m1r2)\mathbf{M} = \begin{pmatrix} M_{rr} & M_{r\varphi} \\ M_{\varphi r} & M_{\varphi\varphi} \end{pmatrix} = \begin{pmatrix} m_1 + m_2 & 0 \\ 0 & m_1 r^2 \end{pmatrix}

This matrix summarizes how the system's kinetic energy (TT) depends on the generalized velocities (r˙\dot{r} and φ˙\dot{\varphi}), where T=12(r˙ φ˙)M(r˙φ˙)T = \frac{1}{2} (\dot{r} \ \dot{\varphi}) \mathbf{M} \begin{pmatrix} \dot{r} \\ \dot{\varphi} \end{pmatrix}.

The components, have the following physical meanings:

Mrr=m1+m2 M_{rr} = m_1 + m_2

  • Meaning: This is the total mass of the system.

  • Reason: Since both mass m1m_1 (on the plane) and mass m2m_2 (hanging below) move together with the radial velocity r˙\dot{r} (as m2m_2 moves vertically only when rr changes), they both contribute fully to the effective inertia for radial motion.

Mφφ=m1r2 M_{\varphi\varphi} = m_1 r^2

  • Meaning: This is the moment of inertia of mass m1m_1 alone.

  • Reason: Only the mass m1m_1, which is free to move in the horizontal plane, rotates about the central zz-axis (the hole). Mass m2m_2 is constrained to move purely vertically (radially) and does not contribute to the angular kinetic energy term (φ˙2\dot{\varphi}^2), so it is excluded from MφφM_{\varphi\varphi}.

Mrφ=Mφr=0 M_{r\varphi} = M_{\varphi r} = 0

  • Meaning: The cross-terms are zero, confirming that the generalized coordinates ( rr and φ\varphi) are uncoupled in the kinetic energy.

  • Reason: As shown by the grouping of terms in the total kinetic energy expression, T=12(m1+m2)r˙2+12(m1r2)φ˙2T = \frac{1}{2} (m_1 + m_2) \dot{r}^2 + \frac{1}{2} (m_1 r^2) \dot{\varphi}^2, there is no mixed-product term proportional to r˙φ˙\dot{r} \dot{\varphi}. This zero result simplifies the subsequent Lagrangian dynamics equations, as radial acceleration is not directly dependent on angular velocity, and vice-versa (in terms of kinetic energy).

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