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Calculators

Moment of Inertia (Solid Sphere)

Computes I=0.4·m·r² for a solid sphere spinning about an axis through its center.

Moment of inertia of a sphere

Spin a solid sphere of mass M and radius R about a diameter and you get I = (2/5)·M·R². Make it hollow instead — a thin spherical shell — and the figure climbs to I = (2/3)·M·R². Plug in M = 5 kg and R = 0.2 m and the solid case works out to I = 0.4·5·0.04 = 0.08 kg·m². The Earth is close to a sphere too, but its core is far denser than its outer layers, so the moment of inertia we actually measure comes out to I ≈ 0.33·M·R², below 2/5. That drop is the signature of mass piling up near the middle.

There's a classic demo for this. Roll a solid ball and a hollow one of matching mass and radius down the same incline. The hollow ball, with its larger I, crosses the finish line last, since a bigger share of its energy is tied up in spinning rather than moving forward.

Applications: planets, gyroscopes and rolling experiments

Measure a planet's moment of inertia and you can read its insides: Earth's 0.33, against the 0.4 of a uniform ball, points straight to a dense core, and geophysicists lean on that kind of comparison. Gyroscopes, ball bearings, bowling balls — how each one behaves when it rotates traces back to I. The ramp experiment keeps showing up in physics labs for a good reason. The (2/5)MR² of a solid sphere predicts an acceleration of a = (5/7)·g·sinθ, a touch below what the (2/3) hollow sphere gives, and a stopwatch is enough to tell them apart.

FAQ

Why is (2/3) larger than (2/5)? Every bit of the hollow shell sits out at radius R. The solid sphere instead spreads its mass across the whole range from 0 to R, which pulls down the average r² weighting in I = ∫r² dm.

What is Earth's moment of inertia coefficient? Satellite tracking puts it at roughly 0.3307·M·R². It falls short of 0.4 because the iron core packs far more density than the mantle around it.

Does I depend on the axis? Not for a uniform sphere: thanks to its full symmetry, any axis you draw through the centre yields the same I. Once a body stops being spherical or starts to be layered, that no longer holds.

Which rolls faster, solid or hollow? The solid one. It carries less I per kg·R², so more of the gravitational PE ends up as translational KE rather than spin.

Related Tools

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Sphere Moment of Inertia

Compute solid sphere (I = 2/5·m·r²) or hollow shell (I = 2/3·m·r²) moment of inertia.

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Moment of Inertia (Solid Cylinder)

Computes I=0.5·m·r² for a solid cylinder spinning about its central axis.

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Rectangular Section Inertia

Compute Ix and Iy of a rectangular section: Ix = b·h³/12, Iy = h·b³/12. Also section modulus W.

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Torque for Angular Acceleration

Calculate the torque needed to angularly accelerate a rotating body, T = I·α, from the moment of inertia I and the desired angular acceleration α (rad/s²). The result, in N·m, is the rotational version of Newton's second law (F = m·a): the greater the assembly's inertia or the faster the intended acceleration, the more torque the motor must provide. It is fundamental in sizing drives that must accelerate and decelerate loads quickly — robots, positioners, spindles — where the acceleration torque adds to the friction and load torque. Enter the moment of inertia and the angular acceleration.

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Angular Momentum L=I·ω

Calculates angular momentum L in kg·m²/s from moment of inertia I and angular velocity ω in rad/s.

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Rotational Braking Time

Calculate the time to brake (stop) a rotating system, t = (I·ω) ÷ T, from the moment of inertia I (kg·m²), the initial angular velocity ω (rad/s) and the braking torque T (N·m). When a brake applies a constant torque to a spinning system (a shaft, flywheel, machine rotor), it DECELERATES it to a stop. By Newton's second law for rotation (T = I·α, with α the angular deceleration), the stopping time is the initial angular momentum (I·ω) divided by the braking torque. This matters in several situations: EMERGENCY STOPPING of machines (safety codes require dangerous parts to stop within a maximum time after brake actuation — the shorter, the safer), sizing motor and shaft brakes, and clutches (the engagement time, where the clutch 'synchronizes' two shafts' speeds, follows the same physics). Systems with large moment of inertia (heavy flywheels, big rotors) take longer to stop with a given torque — so high-inertia machines need powerful brakes or more stopping time. The braking time, with the dissipated energy and power, completes a braking analysis. Enter the moment of inertia, the angular velocity and the braking torque.

The results provided by this tool are for general informational and educational purposes only and do not constitute professional, financial, medical, legal, tax or accounting advice. Always confirm important decisions with a qualified professional and official sources.