Static equilibrium for a rope on a spool. Same as A+55+5.
1K10.30 • A+60+35

Static Equilibrium of a Spool. Tension = T = mg. If T is not too large, the spool will roll without slipping. It will reach equilibrium at angle given by: sin(theta)= R1 / R2. If T is increased, the spool will start to slip, but the angle will stay the same. Derivation: Equilibrium: F = T sin(theta) Rotation: F R1 = T R1 Divide one equation by the other: 1/ R2 = sin(theta) / R1. Table Stand R1= 94mm R2= 203mm
Related Demos
A+60+0
Meterstick suspended in mid-air by horizontal strings and weights. A+60+5
Force on hinged beam measured with transducer. A+60+10
Forces on crane boom measured with transducer. A+60+15
Two transducers measure forces from centered hanging mass. A+60+16
Same as A+60+15, but mass in different position. A+60+20
Car hangs balanced by forces in mid-air over removable inclined plane. A+60+25
Disk (weighted off-center) rolls up inclined plane. A+60+30
Irregular shapes to determine center of mass using plumb bob. A+60+32
Center of gravity (toy) objects. A+60+37
Rotation about the center of mass: Object to throw. A+60+40
Anatomical models: Skull, Arm, Leg A+60+22
Tensegrity: The Impossible Table A+60+60
Stability of ladder depends on weight distribution A+60+45
Center of mass of a baseball bat A+60+50
Applet: Motion of the Center of Mass A+60+55
Stacking Blocks Extend Over Base