aθ = 2 · ω · vr
A body sliding in a rotating radial slot has a transverse Coriolis acceleration in addition to its radial motion.
A body sliding in a rotating radial slot has a transverse Coriolis acceleration in addition to its radial motion.
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A body sliding in a rotating radial slot has a transverse Coriolis acceleration in addition to its radial motion.
With ω = 2 rad/s and outward sliding speed vr = 1 m/s, aθ = 2·2·1 = 4 m/s² across the guide.
Planar motion in a rigid radial guide about a common axis; aθ is only the Coriolis contribution to absolute acceleration. Centripetal, angular-acceleration and relative-acceleration terms require separate addition. General three-dimensional motion uses 2Ω×vrel.
A slider moves along a radial guide while the guide rotates. This calculator finds the extra lateral acceleration caused by that combined motion.
Coriolis acceleration is the part of absolute acceleration caused by simultaneous rotation of the guide and motion relative to it. For a radial slot, aθ = 2ωvr. Here ω is guide angular velocity, vr radial relative speed, and aθ transverse acceleration. Positive ω means counter-clockwise rotation and positive vr means outward motion; a negative result points in the opposite circumferential direction.
aθ = 2 · ω · vr
Radial guide: aθ = 2ωvrGeneral vector form: aC = 2Ω×vrel| Symbol / input | Meaning |
|---|---|
| Transverse acceleration aθ | Signed Coriolis acceleration across the radial guide; positive is the circumferential direction for positive ω. Multiply by mass to estimate lateral guide force. |
| Angular velocity ω | Angular speed of the guide about its axis from speed data or measurement; positive counter-clockwise. |
| Relative radial sliding speed vr | Body speed relative to the guide along the radial slot; positive outward, negative toward the rotation axis. |
ω in rad/s comes from speed measurement or drive data: ω = 2πn/60 when n is in revolutions per minute. vr in m/s is sliding speed measured relative to the guide, for example from a displacement-time record. Either input may be positive, zero or negative to represent direction. aθ in m/s² is transverse acceleration; multiplying it by slider mass gives an estimate of lateral contact force.
Define positive rotation and radial directions. Enter angular velocity and relative sliding speed at the same instant. Read output sign using those conventions, and add the remaining motion terms separately when finding total absolute acceleration.
A guide rotates counter-clockwise at ω = 2 rad/s. A slider moves outward at vr = 1 m/s: aθ = 2·2·1 = 4 m/s² in the positive circumferential direction. With vr = −1 m/s the result is −4 m/s².
No guide rotation or no relative sliding gives zero Coriolis acceleration. Doubling ω or vr doubles aθ. The acceleration is perpendicular to radial sliding speed.
The internal units are rad/s for ω, m/s for vr and m/s² for aθ. One revolution per minute equals 2π/60 rad/s; the existing SI registry handles unit conversion.
Early estimates of lateral slider loads in rotating guides, crank mechanisms and rotating test rigs.
The relation assumes planar motion in a rigid, exactly radial guide and returns only the Coriolis term. Centripetal acceleration, angular acceleration of the guide and relative acceleration along the guide are excluded. Inclined or spatial motion needs the vector form 2Ω×vrel.
Common mistake: Do not enter absolute body speed as vr: vr is speed relative to the rotating guide alone. Do not confuse the result with centripetal acceleration ω²r, which depends on radius rather than sliding speed.
Early estimates of lateral slider loads in rotating guides, crank mechanisms and rotating test rigs.
ω in rad/s comes from speed measurement or drive data: ω = 2πn/60 when n is in revolutions per minute. vr in m/s is sliding speed measured relative to the guide, for example from a displacement-time record. Either input may be positive, zero or negative to represent direction. aθ in m/s² is transverse acceleration; multiplying it by slider mass gives an estimate of lateral contact force.
The relation assumes planar motion in a rigid, exactly radial guide and returns only the Coriolis term. Centripetal acceleration, angular acceleration of the guide and relative acceleration along the guide are excluded. Inclined or spatial motion needs the vector form 2Ω×vrel.