Normalize a radial density before integrating disk inertia
Distinguish circumference, area density and rotational distance in a continuous inertia calculation.
Learning outcome: At R=2 compare n=0,2,4. Derive sigma 0 before I, retain normalized shape factors and compare the thin-rim limit. Explain which extra geometric factor appears for a spherical shell.
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Declare the fixed axis, integrate the actual mass or load distribution, and test constraint feasibility before interpreting a numerical result.
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M=2,R=2,n=2 gives sigma 0=1/pi kg/m² and I=16/3 kg m². At the same mass/radius, the uniform disk gives 4 and the thin hoop 8.
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When changing radial density shape at fixed mass, may sigma 0 remain unchanged?
Experiment
At R=2 compare n=0,2,4. Derive sigma 0 before I, retain normalized shape factors and compare the thin-rim limit. Explain which extra geometric factor appears for a spherical shell.
Integrate annular mass with fixed total mass
Worked teaching model · synthetic values · Thin disk mass 2 kg, sigma=sigma0(r/R)^n normalized to the same mass. Axis perpendicular through center; dm=2pi r sigma dr. No axial thickness or actual machining.
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Annular inertia integrand
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Annular inertia integrand: numerical coordinates
| radius (m) | dI/dr (kg m) |
|---|---|
| 0 | 0 |
| 0.05 | 1.56250e-7 |
| 0.1 | 5.00000e-6 |
| 0.15 | 3.79687e-5 |
| 0.2 | 0.00016 |
| 0.25 | 0.000488281 |
| 0.3 | 0.001215 |
| 0.35 | 0.00262609 |
| 0.4 | 0.00512 |
| 0.45 | 0.00922641 |
| 0.5 | 0.015625 |
| 0.55 | 0.0251642 |
| 0.6 | 0.03888 |
| 0.65 | 0.0580145 |
| 0.7 | 0.084035 |
| 0.75 | 0.118652 |
| 0.8 | 0.16384 |
| 0.85 | 0.221853 |
| 0.9 | 0.295245 |
| 0.95 | 0.38689 |
| 1 | 0.5 |
| 1.05 | 0.638141 |
| 1.1 | 0.805255 |
| 1.15 | 1.00568 |
| 1.2 | 1.24416 |
| 1.25 | 1.52588 |
| 1.3 | 1.85647 |
| 1.35 | 2.24202 |
| 1.4 | 2.68912 |
| 1.45 | 3.20487 |
| 1.5 | 3.79688 |
| 1.55 | 4.4733 |
| 1.6 | 5.24288 |
| 1.65 | 6.11491 |
| 1.7 | 7.09928 |
| 1.75 | 8.20654 |
| 1.8 | 9.44784 |
| 1.85 | 10.835 |
| 1.9 | 12.3805 |
| 1.95 | 14.0975 |
| 2 | 16 |
| Quantity | Value | Unit |
|---|---|---|
| Normalized edge density sigma0 | 0.31831 | kg/m² |
| Total fixed mass | 2 | kg |
| Central rotational inertia | 5.33333 | kg m² |
| Shape factor I/(MR²) | 0.666667 | ratio |
| Equal-mass thin-rim inertia | 8 | kg m² |
Annular mass includes the circumference factor before the additional r² inertia weighting.
Integrate dm=2pi r sigma dr to normalize mass first. Then I=integral r²dm gives MR²(n+2)/(n+4). At n=0 the uniform disk factor is1/2; concentrating mass outward increases it toward the thin-rim value1, not beyond it.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
Annular mass includes the circumference factor before the additional r² inertia weighting.
Integrate dm=2pi r sigma dr to normalize mass first. Then I=integral r²dm gives MR²(n+2)/(n+4). At n=0 the uniform disk factor is1/2; concentrating mass outward increases it toward the thin-rim value1, not beyond it.
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Why does a central axis not make every point on a spherical shell equally far from it?
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