Two astronauts, Alice and Bob, are standing inside their cylindrical spaceship, which is rotating at an angular velocity ω clockwise around its axis in order to simulate the gravitational acceleration g on earth. The radius of the spaceship is R. For this problem, we will only consider motion in the plane perpendicular to the axis of the spaceship. Let point O be the center of the spaceship. Initially, an ideal zero-length spring has one end fixed at point O, while the other end is connected to a mass m at the "ground" of the spaceship, where the astronauts are standing (we will call this point A ). From the astronauts' point of view, the mass remains motionless.
Next, Alice fixes one end of the spring at point A, and attaches the mass to the other end at point O. Bob starts at point A, and moves an angle θ counterclockwise to point B (such that AOB is an isosceles triangle). At time t=0, the mass at point O is released. Given that the mass comes close enough for Bob to catch it, find the value of θ to the nearest tenth of a degree.
Assume that the only force acting on the mass is the spring's tension, and that the astronauts' heights are much less than R.
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Given constants:
- Proton mass, mp=1.67⋅10−27kg
- Neutron mass, mn=1.67⋅10−27kg
- Electron mass, me=9.11⋅10−31kg
- Avogadro's constant, N0=6.02⋅1023mol−1
- Universal gas constant, R=8.31J/(mol⋅K)
- Boltzmann's constant, kB=1.38⋅10−23J/K
- Electron charge magnitude, e=1.60⋅10−19C
- 1 electron volt, 1eV=1.60⋅10−19J
- Speed of light, c=3.00⋅108m/s
- Universal Gravitational constant,
G=6.67⋅10−11(N⋅m2)/kg2
- Solar Mass
M⊙=1.988⋅1030kg
- Acceleration due to gravity, g=9.8m/s2
- 1 unified atomic mass unit,
1u=1.66⋅10−27kg=931MeV/c2
- Planck's constant,
h=6.63⋅10−34J⋅s=4.41⋅10−15eV⋅s
- Permittivity of free space,
ϵ0=8.85⋅10−12C2/(N⋅m2)
- Coulomb's law constant,
k=4πϵ01=8.99⋅109(N⋅m2)/C2
- Permeability of free space,
μ0=4π⋅10−7T⋅m/A
- Magnetic constant,
4πμ0=1⋅10−7(T⋅m)/A
- 1 atmospheric pressure,
1atm=1.01⋅105N/m2=1.01⋅105Pa
- Wien's displacement constant, b=2.9. 10−3m⋅K
- Stefan-Boltzmann constant,
σ=5.67⋅10−8W/m2/K4