1. Solve for the initial tangental velocity of both drops (V0 and V1 )
use: (Vfinal)2 = (Vinitia)l2 + 2 α Δr
Vfinal = will be zero when the drop reaches highest point. Solve for Vinitial
V0 initial = √(2 (9.8) (.542) = 3.26 m/s
V1 initial = √(2 (9.8) (.510) = 3.16 m/s
2. Solve for ω (angular velocity):
ω = V /radius
ω0 = 3.26 / .357 = 9.13 radians / second
ω1 = 3.16 / .357 = 8.85 radians / second
3. Solve for α (angular acceleration) using circular motion kinematics:
(ωfinal)2 = (ωinitial)2 + 2 α Δθ
8.852 = 9.132 + 2 α 2π
78.3-83.4 = 4π α
4πα = -5.1
α = -.406 radians/ second2
The magnitude of acceleration would be .406 radians/ second2
A bicycle is turned upside down while its owner repairs a flat tire. A friend spins the other wheel, of radius 0.357 m,...
- 8. QC A bicycle is turned upside down while its owner repairs a flat tire. A friend spins the other wheel and observes that drops of water fly off tangentially. She measures the heights reached by drops mov- ing vertically (Fig. P7.8). A drop that breaks loose from the tire on one turn rises vertically 54.0 cm above the tangent point. A drop that breaks loose on the next turn rises 51.0 cm above the tangent Figure P7.8 Problems...
8. QIC A bicycle is turned upside I--- down while its owner repairs a flat tire. A friend spins the other wheel and observes that drops of water fly off tangentially. She measures the heights reached by drops mov- ing vertically (Fig. P7.8). A drop that breaks loose from the tire on one turn rises vertically 54.0 cm above the tangent point. A drop that breaks loose on the next turn rises 51.0 cm above the tangent Figure P7.8 Problems...