Absolutely agree. And this is probably as good a place as any to post an analysis of the model Wilkins provided a while back. I bet most of those on the other side of this issue have not bothered to do any analysis of it. If you do, it shows exactly what you are saying above:
1 1 Vg 1 1 1 1 ohm ------R1-- Rw----------Rg-----------Rg--------Rw --- R2------ ! ! = ! ! ! = ! PV V1 Rload 100 ohms V2 240V array ! ! = ! ! ! = ! =20---------------------------------------------------------------------------
Here's a simple model of what we have. V1 and R1 are a Thevinin model of the PV array. R1 is the internal resistance of the PV array. Rw is the resistance of the wire connecting the array to the grid. Rg is the resistance of the grid wire connecting the load two blocks away. That load is driven by another power source in parallel, modeled by V2 and R2, it;s connecting wire Rw. I hope we can all agree that this is a valid model for the discussion at hand.
Step 1: The sun is not shining, the PV is supplying no current. What is the voltage at the grid connection point Vg? We know the only current flowing is from V2. That current is 240/(100+1+1+1) =3D 240/103=3D 2.33 amps. That current flows through the Rload resistor producing a voltage of 100 X 2.33 =3D 233 volts across the load. Since we know zero current is flowing in the left side of the circuit, the current through R1, R2, Rw must be zero. The only way for that to occur is for Vg to be equal to 233 volts. The grid voltage is now 233 volts. The voltage at V1 must also be 233 volts.
Step 2: The sun comes out and the PV is going to put it's power on the grid. The only way for current to start flowing through V1 is for V1 to INCREASE above 233 volts. As it does, the voltage on the grid will slowly increase too. How do we know this? Let's look at the simplest case, where the PV array can supply half the total current. Writing the Kirchoff equation for the right side of the loop we have:
240 =3D i2 x (R2 + Rw + Rg) + (i1 + i2) x Rload240 =3D i2 x 3 + ( i1 + i2) x 100
240 =3D 100 x i1 + 103 x i2Where i2 is the current flowing from source V2 and i1 is the current flowing from the PV array. We also know that each source is supplying half the current, so i1 =3D i2. Substituting, we have
240 =3D 100 x i1 + 103 x i1240 =3D 203 i1
or i =3D 1.182 amps.
We know that twice that is flowing through the load, so the voltage across the load is 100 x 1.182 x 2 =3D 236.4 volts
Before we brought V1 online it was 233 volts. Now it is
3.4 volts HIGHER. Intuitively this makes sense, because the voltage there must RISE enough to reduce the current that was flowing from the other power source V2.Now that we have the voltage across the load, and know that I1 is 1.182 amps we can calculate the voltages at the grid, Vg and what V1 must be:
Vg =3D 236.4 + i1 x Rg =3D 236.4 + 1.182 =3D 237.6 volts
V1 =3D 236.4 + i1 x (Rg + Rw+ R1) =3D 236.4 + 1.182 x 3 =3D 239.9 volts
All the voltages along the way have increased, the voltage at the load, the voltage at the grid, and the voltage at the PV array.
QED