|
Size: 1489
Comment:
|
Size: 1503
Comment:
|
| Deletions are marked like this. | Additions are marked like this. |
| Line 20: | Line 20: |
| . Test the Vernikos theory: do healthy humans do '''better'' in > 1 gee environments? | . Test the Vernikos theory: do healthy humans do '''better''' in > 1 gee environments? |
| Line 28: | Line 28: |
| $ a = 9.81 \times gee = \omega^2 R = { \Large { { 2 \pi } \over T }^2 } R = 4 \pi^2 { \Large { R \over T^2 } } ~~~ T $ in seconds | $ a = 9.81 \times gee ~=~ \omega^2 R ~=~ { \Large \left( { 2 \pi } \over T \right) }^2 R ~=~ 4 \pi^2 { \Large { R \over T^2 } } ~~~ T $ in seconds |
| Line 30: | Line 30: |
| $ gee \times T^2 \approx 4 R ~~~~~ T = 60 / RPM $ | $ gee \times T^2 \approx 4 R ~~~~~ T ~=~ 60 / RPM $ |
| Line 32: | Line 32: |
| $ R = { \Large \left( 30 \over RPM \right)^2 } gee $ |
$ R ~=~ { \Large \left( 30 \over RPM \right)}^2 gee $ |
Gee Plus
Adapting to a High RPM Environment
The Experiment
A 36 meter radius, rotating long-duration space habitat simulation on Earth, simulating 1.4 gees at 10 RPM. 1.4 gees is the vector sum of 1 gee horizontal and 1 gee vertical. Experimental subjects with BMI < 20, having a "gravitational BMI" < 28 but the same "metabolic BMI".
Postulates
1 Humans evolved to run, hence may be optimized for > 1 gee
- see work by Joan Vernikos, NASA Ames (retired)
- zero gee causes rapid "aging"
- 2 The human vestibular system can adapt to high RPMS
- Experiments with rotating rooms show 6 RPM adaptation in 3 days, 10 RPM in 5 days
Experiments with rotating tube beds suggest 30 RPM
adaptation for head movements - Athletes undergo much faster head rotations
Goals
Test the Vernikos theory: do healthy humans do better in > 1 gee environments?
- Learn about long term vestibular adaption, and the transition from rotation to non-rotation
- frequent transitions through the hub to 1 gee and 0 RPM
- Select astronauts for vestibular tolerance for rotating habitats in microgravity
- Make low BMI people into heros
Math
a = 9.81 \times gee ~=~ \omega^2 R ~=~ { \Large \left( { 2 \pi } \over T \right) }^2 R ~=~ 4 \pi^2 { \Large { R \over T^2 } } ~~~ T in seconds
gee \times T^2 \approx 4 R ~~~~~ T ~=~ 60 / RPM
R ~=~ { \Large \left( 30 \over RPM \right)}^2 gee