Transfer efficiency of energy is the keystone to this
project. If we can’t transfer kinetic energy of one branch to the other, we’re
just dumping gigawatts into Entropy.
There is no data readily available on possible energy
transfer efficiencies, although I have far from performed due diligence.
Instead, let’s look at the implications of different hypothetical transfer
efficiencies.
The only thing we have on our side here is potential energy, stored in the form of dense rock at high elevation. In an ideal situation (perfectly frictionless track, complete transfer of kinetic energy from incoming cargo to outgoing cargo), the scenario looks something like this:
Once the system is brought up to
full speed, 96% of the power at each station is transferred to accelerate the
outgoing cargo. The remaining 4% is transferred to usable energy. Based on full
output, this results in a generation of 64 GW.
Of course, ideal conditions are not possible. While
VacMagLev has minimal friction losses in transit, we have to assume that some
of our power generated by regenerative braking will be lost to entropy. How
much power loss greatly affects the system’s performance.
In the following examples, we lower the operating capacity
of the line. Since energy is proportional to the square of velocity, and
operating efficiency is assumed as a constant regardless of energy use, a
lower-velocity system should see significantly less entropy. Also note there is
an additive effect of these efficiencies. At a 90% transfer efficiency, we experience
losses in one cycle of the Colorado – New Orleans – Lake Superior hub of
1 –
(0.90*0.90*0.90) = 27%
For each assumed energy transfer efficiency, we look at two
scenarios: first, what is the maximum system velocity that will leave us with
an energy-neutral system. Secondly, what is a reasonable system velocity that
also produces energy? Results are as follows:
|
Energy Transfer Efficiency |
Velocity with 0 power consumption, m/s |
Design Velocity & Design power generation |
|
100% |
--- |
900 m/s, 64 GW |
|
95% |
812 |
750 m/s, 9 GW |
|
90% |
601 |
350 m/s, 12 GW |
|
85% |
457 |
300 m/s, 6 GW |
|
80% |
327 |
200 m/s, 3 GW |
|
70% |
28 |
--- |
|
50% |
--- |
--- |
It’s almost laughable that we consider 200 m/s and 3 GW as modest, but that’s exactly what we can get if we can improve kinetic energy transfer to 80%.