 Near Earth's surface, a free falling object will accelerate at rate g, approx. 9.8 m/sec2.
Thus, an acceleration of 10 g
would be about 98.1 m/sec2.
Using Newtonian motion equations, we previously determined the first second of 1-g free fall will move object 4.9 meters. Extend to one day of constant g-force acceleration to move vessel to .245 Astronomical Units (AUs).
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Expand our thought experiment's envelope to exceed g-force acceleration for selected vessels. Assume no humans, but Artificial Intelligence (AI) devices will guide a vessel with essential cargo.
Express 10g differently.
10g | ≈ | 98.065 m
sec2 | × | (86,400 sec)2
day2 |
× | 1 AU
149,597,870,700 m | ≈ | 10g ≈ | 4.893 AU
day2 |
If double g-force does not damage ship or contents; then, much shorter travel time would be an enormous benefit.
d | = | a×t2
2 | ≈ | 4.893 AU
day2 | × | (1 day)2
2 | = | 2.45 AU |
let a = 10g = 4.893 AU/day²
NOTE: 1 sec of 10-g acceleration moves an object 49.1 m; thus, extend to 1 day (86,400 sec) for distance of 2.45 AU.
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First Day of i×G-force Propulsions
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Describe greater accelerations as integer (i) times g, gravity force experienced on Earth's surface.
DISTANCE EXAMPLE: After one day of 10g-force acceleration, object travels a great distance:
dAccel = .5 × a × t2 = .5 × 10g × t2 = .5 × 10(.245AU/day2) × day2 = 2.447 AU
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Attain Great Speeds with 1-G Propulsion
Re-express light speed, c
c | = | 299,792.458 km
sec | = c × | AU
149,597,871 km |
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| × | 86,400 sec
day |
|
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| = | 173.145 AU
day |
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Daily Difference:
Δ1-G | = | VDay
c |
|
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| = | .489 AU/day
173.145 AU/day | = | 0.283% c |
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Daily Remainder: (1 - Δ)
R1-G | = | c (1 - Δ1-G) = | | c(1-.00283) | | = | .99717 c |
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Previous work shows Vt = c(1 - Rt)
Time
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Einsteinian
Velocity
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Newtonian
Velocity
|
Days
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% Light Speed
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AU/Day
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AU/Day
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1
|
0.283% c
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0.490
| 0.490 |
5
|
1.407% c
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2.436
| 2450 |
10
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2.794% c
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4.838
| 4.900 |
t
|
c (1-Rt)
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Convert
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t × a1-G
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Show Einsteinian velocities as both percent light speed (%c)
and equivalent AUs per day.
For lesser velocities, Einstein and Newton velocities are fairly close.
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Much Greater Speeds with 10 G Propulsion
Daily Difference for 10g propulsion
Δ10G= 10× 0.283%c = 2.83%c |
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Daily Remainder for 10g propulsion
R10G | = | c (1 - Δ10G) = | | c(1-.0283) |
| = | .9717 c |
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For 10g propulsion, let R = .9717.
Time
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Einsteinian
Velocity
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Newtonian
Velocity
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Days
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% Light Speed
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AU/Day
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AU/Day
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1
|
2.830% c
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4.838
| 4.838 |
5
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13.371% c
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23.152
| 24.190 |
10
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24.955% c
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43.208
| 48.380 |
t
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c (1-Rt)
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Convert
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t × a10G
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After 10 days of 10-g propulsion,
Einsteinian velocity significantly differs from Newtonian velocity.
TE assumes Einsteinian velocity is more accurate. See next table.
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Velocities for Different Super-G's
Accel. | a = 1 × g | a = 4 × g | a = 7 × g | a = 10 × g |
Daily Diff. | Δ = .2826%c | Δ = 1.1305%c | Δ = 1.9784%c | Δ = 2.826%c |
Daily Rem. | R = 99.7174% | R = 98.8695% | R = 98.0216% | R = 97.1738% |
Time (t) | Einstein | Newton | Einstein | Newton | Einstein | Newton | Einstein | Newton |
AU/day | AU/day | AU/day | AU/day | AU/day | AU/day | AU/day | AU/day |
1 day |
0.489
| 0.489 | 1.957 | 1.957 | 3.425 | 3.425 | 4.893 | 4.893 |
10 days | 4.832 | 4.893 | 18.608 | 19.574 | 31.360 | 34.254 | 43.158 | 48.935 |
100 days | 42.68 | 48.93 | 117.60 | 195.74 | 149.67 | 342.54 | 163.70 | 489.35 |
200 days | 74.84 | 97.87 | 155.33 | 391.48 | 169.96 | 685.09 | 172.58 | 978.69 |
300 days | 99.07 | 146.80 | 167.43 | 587.22 | 172.71 | 1,027.63 | 173.11 | 1,468.04 |
365¼ days | 111.56 | 178.73 | 170.42 | 714.92 | 173.03 | 1,251.14 | 173.14 | 1,787.34 |
400 days | 117.33 | 195.74 | 171.31 | 782.96 | 173.09 | 1,370.17 | 173.14 | 1,957.39 |
Given |
Vt = c × | (1 - Rt) | 173.145 AU/day
c |
Einsteinian Velocities
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Vt = t × a = t × i×g = | t × i × | 0.489 AU
day² |
Newtonian Velocities
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For even faster interstellar cargo transport, consider super G-forces even greater than 1g. With acceleration as i × g, table considers integer "i" values as high as 10.Newtonian method computes velocities greater than light speed (c=173.145 AU/day) ; IMPOSSIBLE!!!! Thus, Thought Experiment proposes Einsteinian Velocities for subsequent use.
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Interstellar Distances for Different Super-G's
Accel. | a = 1 × g | a = 4 × g | a = 7 × g | a = 10 × g |
Daily Diff. | Δ = .2826%c | Δ = 1.1305%c | Δ = 1.9784%c | Δ = 2.826%c |
Daily Rem. | R = 99.7174% | R = 98.8695% | R = 98.0216% | R = 97.1738% |
Time (t) | Velocity | Distance | Velocity | Distance | Velocity | Distance | Velocity | Distance |
%c | LY | %c | LY | %c | LY | %c | LY |
1 day |
0.28%
| 0.0000039 | 1.13% | 0.0000155 | 1.98% | 0.00003 | 2.83% | 0.00004 |
10 days | 2.79% | 0.00038 | 10.75% | 0.00150 | 18.11% | 0.00256 | 24.93% | 0.00358 |
100 days | 24.65% | 0.035 | 67.92% | 0.110 | 86.44% | 0.155 | 94.31% | 0.184 |
200 days | 43.22% | 0.129 | 89.71% | 0.332 | 98.16% | 0.413 | 99.68% | 0.452 |
300 days | 57.22% | 0.268 | 89.71% | 0.589 | 99.75% | 0.685 | 99.98% | 0.726 |
365¼ days | 64.43% | 0.377 | 98.43% | 0.763 | 99.93% | 0.863 | 99.9972% | 0.905 |
400 days | 67.76% | 0.440 | 98.94% | 0.857 | 99.97% | 0.958 | 99.9990% | 0.999999 |
Given |
Vt = (1 - Rt) | × | c |
Einsteinian Velocities
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dt = | c × t | + | Vt
ln(1-Δ) |
Einsteinian Distances
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For even faster interstellar cargo transport, consider super G-forces even greater than 1g. With acceleration as i × g, table considers integer "i" values as high as 10.Thought Experiment proposes Einsteinian Velocities and Distances.
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Interstellar Fuel Flow
Relativistic fuel particles grow in mass which further increases momentum of exhaust flow.
EXAMPLE: Let one second of consumed fuel flow, ffsec, be 1,000 gms of at rest water particles. Accelerate these particles to a relativistic exhaust velocity ( VExh) of .992 light speed.
VExh = dc×c =.992c = 99.2% light speed
As shown in the right hand panel, 1.0 kg of ffsec will grow to become 8.0 kgs of exhaust fuel flow, ffExh, just before it exits vessel and contributes to forward momentum. NOTE: Consume fuel particles at rest; expel at relativistic speeds.
ffExh = n × ffsec
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For convenience, note following identities:
Growth Factor
n
|
=
| 1
√(1 - dc2) |
Growth Factor (n)
Uses Lorentz Transform (LT) as shown.
Decimal Component (dc)
If particle speed is expressed as decimal light speed; then, dc is the decimal portion.
Decimal Component
dc | = | √(n2 - 1)
n |
LT can be rewritten
to solve for dc (see table at right).
Thus, conveniently generate below table.
Growth
Factor (n) | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 |
Fuel Exhaust
Speed(dc×c) | 0.00c | .866c | .942c | .968c | .980c | .986c | .990c | .992c |
For convenience, n is expressed as series of integers,
but n could also be a rational number greater than 1.
To discuss following tables,
TE arbitrarily assumes a relativistic growth factor of 8.
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Theoretical Daily Diff: (∇E=1)
Consistent acceleration ever increases daily velocities and daily distances; it also requires daily fuel,
best expressed as a percentage of ship's gross weight (%GW).
First, consider daily diff with 100% Efficiency (∇E=1),
a misconception, soon corrected.
Determine ratio
of daily fuel
to Ship's Mass
∇E=1= | 86,400 × ffSec
MShip |
Daily fuel = 86,400 seconds
of at-rest fuel consumption
To determine ship's mass:
Recall Momentum Exchange
Huge mass of ship × small velocity increase =
tiny collective mass of fuel exhaust particles × huge relativistic velocity.
MShip × VShip = MExh × VExh |
Divide each side by one second for useful restatement.
MShip × VShip
sec | = |
MExh × VExh
sec |
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Substitute and re-arrange:
Equal Forces
MShip × AShip = ffExh × (dc × c) |
State ship's acceleration (AShip) as multiple of g, Earth's gravity:
Equal Forces Restated
MShip × (i × g ) = (n ×ffsec) × (dc × c) |
∇E=1= | ffDay
Mship | = | 86,400 × ffSec
n×ffSec×dc×c/(i×g) |
Solve for Ship's mass (Mship) and substitute:
∇E=1 = | ffDay
Mship | = | 86,400 ×i×g/c
n × dc |
Further simplify:
Recall decimal component in terms of n, growth factor:
Make following substitutions:
Light speed, c = 299,792,458 m/sec
Earth gravity, g = 9.8065 m/sec²
Make following substitutions:
Growth factor, n = 8
√(n2-1) = 7.937
Gravity
Mult (i) | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 |
Exhaust
Flow (∇) | 0.0356% | 0.0712% | 0.1068% | 0.1424% | 0.1780% | 0.2136% | 0.2492% | 0.2848% |
If perfectly efficient vessels were possible; then, a 7g-force vessel could use 1% of it's GW for 4 days propulsion. However, we must also consider
INEVITABLE INEFFICIENCIES!!
TE proposes a coefficient {efficiency factor (ε)} to increase fuel consumption (∇ ) to cover both the Exhaust Flow (ffExh=n×ffsec) and inevitable particle losses: design flaws and peripheral systems.
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Synchrotronic Propulsion System will have inevitable inefficiencies. However, they will improve over time.
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Inefficiency (E'= loss/input) reflects the inevitable loss of consumed fuel particles which will not exit the vessel to contribute to ship's velocity increase. This loss may be intentional such as particles diverted for other services. Loss may be unintentional due to design flaws. TE assumes that subsequent designs will decrease particle loss.
Interplanetary Inefficiency: TE assumes 50%.
Interstellar Efficiency must be much better than interplanetary; thus, TE assumes constant tech improvement correlating to n, growth factor. (For following examples, let n = 8.)
E' = (.5 × .9n-2) = .2657
Efficiency, E, can be stated as complement of Inefficiency, E'.
E = 1 - E' = 1 - (.5×.9n-2) = .7347
Efficiency Factor (ε) is a necessary coefficient of daily exhaust flow (∇). As the reciprocal of Efficiency, ε always exceeds one:
ε = | 1
1 - (.5×.9n-2) | = 1.362 |
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Interstellar Daily Difference
Efficiency Factor (ε) helps flight planners account for inevitable inefficiencies.
Gravity
Mult (i) | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 |
Daily
Diff. (ε×∇) | 0.0468% | 0.0936% | 0.1404% | 0.1872% | 0.1872% | 0.2808% | 0.3276% | 0.3744% | 0.4212% | 0.4680% |
Given 7g acceleration, 1% ship's gross weight will provide about 3 day's propulsion.
Interstellar Fuel Consumption for G and Super-G
Accel. | a = 1 × g | a = 7 × g |
Daily Diff. | ε∇ = .0468% GW | ε∇ = .339% GW |
Daily Rem. | (1-ε∇) = 99.9532% GW | (1-ε∇) = 99.61% GW |
Time (t) | Velocity (Vt) | Distance (dt) | Fuel (ft) | Velocity (Vt) | Distance (dt) | Fuel (ft) |
percent c | Light Year | percent GW | % light speed | Light Year | %Gross Wt. |
1 day | 0.28%c | 0.000 003 9 LY | 0.048% GW | 1.98%c | 0.000 03LY | 0.339% GW |
10 days | 2.79%c | 0.000 38 LY | 0.48% GW | 18.11%c | 0.002 56LY | 3.34% GW |
100 days | 24.65%c | 0.035 LY | 4.73%GW | 86.44%c | 0.155LY | 28.82%GW |
200 days | 43.22%c | 0.129 LY | 9.24%GW | 98.16%c | 0.413LY | 49.34%GW |
300 days | 57.22%c | 0.268 LY | 13.54%GW | 99.75%c | 0.685LY | 63.94%GW |
365¼ days | 64.43%c | 0.377 LY | 16.23 %GW | 99.93%c | 0.863LY | 71.11%GW |
400 days | 67.76%c | 0.440 LY | 17.63%GW | 99.97%c | 0.958LY | 74.33%GW |
Given |
Vt = c × |
( 1 - (1-Δ)t )
| |
Einsteinian Velocities
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dt = | c × t | + | Vt
ln(1-Δ) |
Einsteinian Distances
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ft | = |
1 - (1-ε∇)t
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Fuel Consumed
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For even faster interstellar cargo transport, consider 7g acceleration. Assume fuel exhaust particles have velocity, VExh = 99.2%c, with a corresponding growth factor, n = 7.Thought Experiment proposes Einsteinian motions and exponential fuels.
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7g acceleration greatly increases distance and speed much quicker than 1g acceleration;
DOWNSIDE: 7g propulsion requires MUCH MORE FUEL!!!
For more, see "Snowball from Oort". |
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