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From Generator to Socket

Start here. Send the same power down the same line at two voltages and watch ninety-nine per cent of the loss disappear.

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Power is transmitted at very high voltage because loss goes as the square of current, so raising the voltage by a factor of n cuts the loss by n² — and the entire architecture of the grid, including its being AC at all, follows from that one relationship.

The path power takes

StageTypical voltageWhy
Generation11 – 25 kVInsulating a rotating machine for more is impractical
Transmission132 – 765 kVMinimise I²R over hundreds of kilometres
Sub-transmission33 – 66 kVRegional distribution to substations
Distribution11 kVShort distances, many connection points
Consumer415 V three-phase / 240 V singleSafe to be near, and what appliances expect

The voltage goes up and then comes back down, and every transformation costs money. That round trip is the thing the rest of this lesson has to justify.

The calculation that justifies everything

Take 100 MW down a line with 5 Ω of resistance. Line loss is I²R, and I = P/V.

VoltageCurrentLossAs a fraction of 100 MW
11 kV9091 A413 MW413% — impossible
132 kV758 A2.9 MW2.9%
400 kV250 A0.31 MW0.31%

Voltage up 36 times means current down 36 times, and loss down 36² ≈ 1300 times. Transmission at generation voltage is not inefficient; the conductor would vaporise.

Two related facts follow. Loss depends on the current, so it depends on the power factor — reactive current heats the line without delivering anything, which is why power factor correction has an economic value. And loss depends on R, which sets conductor size, which sets tower cost.

Why not higher still

  • Insulation. Clearances, insulator string length and tower dimensions all grow with voltage, and so does the land the corridor needs.
  • Corona. Above a certain surface field the air around the conductor ionises — a real power loss, audible hiss, ozone and radio interference. Bundled conductors exist to reduce the surface gradient.
  • Equipment cost. Transformers, circuit breakers and instrument transformers get sharply more expensive with each insulation class.
  • Ferranti effect. A long, lightly loaded line has receiving-end voltage *higher* than sending-end, because of line capacitance — a problem that grows with voltage and length.

The standard voltages — 132, 220, 400, 765 kV — are not physical constants. They are where the saving on losses stops being worth the cost of insulating for the next step.

Why distribution reverses the argument

Distribution is the same optimisation with different inputs, and it comes out the other way. Distances are a few kilometres, so I²R is small at modest voltage; the number of connection points is enormous, so each one must be cheap; and the clearances that transmission needs cannot exist along a residential street.

This is worth stating explicitly because it is often taught as though low distribution voltage were a compromise. It is the optimum for its own conditions.

Why the system is AC

The whole argument above depends on changing voltage cheaply and efficiently. The only device that does so is a transformer, which needs a changing flux — and therefore AC. A transformer is over 99% efficient, has no moving parts, and lasts decades.

There is a second benefit that is easy to overlook: AC current passes through zero a hundred times a second, and that natural zero is what allows a circuit breaker to interrupt a fault current. Breaking a large DC current is far harder, because there is no moment at which the arc wants to extinguish.

HVDC is used where its converter cost is justified: long submarine cables, where AC charging current would consume the whole rating; very long overhead links; and connecting two grids that are not synchronised with each other.

The constraint no transformer can relieve

A power system stores essentially no energy. What little it has is the rotational inertia of the machines already spinning, and that buys seconds, not minutes.

  1. 1Demand exceeds generation — the extra energy comes out of the spinning machines, and they slow down.
  2. 2Every machine on the grid is electrically locked together, so they all slow together and the frequency falls.
  3. 3Governors sense the fall and open steam or water valves to admit more power.
  4. 4Generation exceeds demand — the machines speed up and the frequency rises, and the process runs in reverse.

So frequency is a continent-wide, real-time measure of supply against demand. It is held within a fraction of a hertz, and a sustained deviation means something serious. This is why load frequency control is a module rather than a footnote.

The numbers you will be asked for

Line loss

P_loss = I²R = (P/V)²·R

The squared term is the entire justification for high-voltage transmission.

Three-phase power

P = √3 · V_L · I_L · cos φ

cos φ is the power factor; reactive current heats the line without delivering power.

Transmission efficiency

η = P_received / P_sent

Typically 92–95% overall from generator to consumer.

Per-unit quantity

value in p.u. = actual / base

Makes transformer ratios vanish from the calculation — which is why every serious analysis uses it.

Advantages and disadvantages

Advantages

  • High-voltage transmission cuts loss by the square of the voltage ratio.
  • Transformers change voltage at over 99% efficiency with no moving parts.
  • An interconnected grid shares reserve, so one station's failure is absorbed by the rest.
  • AC's natural current zero makes fault interruption practical.

Disadvantages

  • Every transformation stage adds capital cost and its own losses.
  • High voltage needs wide corridors, tall towers and land nobody wants to give up.
  • The system stores nothing, so generation must track demand second by second.
  • Interconnection propagates disturbances as well as reserve — which is how cascading blackouts happen.

Watch it work

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Check yourself

question 1 / 5

One question at a time. Pick an answer to see why it is right or wrong, then move on — there is no score to keep and nothing is saved.

Raising transmission voltage from 11 kV to 400 kV cuts the line loss by roughly what factor, for the same power?
If higher voltage is so much better, why is 765 kV about as far as overhead transmission goes?
Why is distribution deliberately done at 11 kV rather than at transmission voltage?
What decided that the grid would be AC rather than DC?
Grid frequency drifts slightly below 50 Hz. What does that tell you?

0 / 5

5 still unanswered — the dots above jump straight to them.

 

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