History of Digital Simulation
RTDS Development Path
History term currents for complex components may require substantial computation
Formulate conductance matrix for equivalent network
Using data from previous timestep (or initial conditions for first timestep), compute new [I] values
Solve for [V] using new values of [I]
Calculate branch currents with [V] and [I]
And repeat…
1
2
3
4
5
Minimal memory requirements
Large number of switches can be represented
All G values can change from timestep to timestep
Current injections
and variable
admittances
Variable admittance elements
● ● ●
Network with n nodes results in admittance matrix n x n in size.
● ● ●
● ● ●
● ● ●
● ● ●
● ● ●
p x p
0
0
m x m
q x q
where L=series inductance &
C=shunt capacitance
T1
T2
T1
T2
Splitting the Network into Subsystems
Traveling wave models (transmission lines or cables) are used to split a network into subsystems
Conductance matrix broken up into block diagonals that can be treated separately
Real Time Simulator
HUT
Signal
output
Signal
input
Mirogrid, Smart Grid and DER
Current Applications
Current Applications
kW – MW range
Current Applications
Current Applications
Guangxi
Three Gorges
34% of GD Load
23.1 GW
8 AC + 5 DC from west to east
8.55GW
7.90GW
Large Scale Simulation
Current Applications
Real time operation
Allow testing of physical controllers
Provide realistic feedback to operators
Physical SCADA interface through DNP3 or IEC 60870-5-104
Black Start Investigation
Current Applications
Future Applications
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