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**GRID ORGANIZATION:**

Electricity systems are inherently government approved monopolies that are ultimately responsible to elected politicians. However, these politicians often mistakingly think that because they understand the law they can manage the complexity of the electricity system. Frequently engineers cannot prevent politicians enacting legislation or approving regulations or setting electricity rates or imposing expenditure constraints that degrade the electricity system. Hence the electricity system design should inherently confine and limit the damage that any single politician or political body can do.

In this respect the electricity system in each political jurisdiction should be able to operate independent of its neighbors. Each political jurisdiction should have sufficient reliable generation in excess of its peak uncontrolled electricity load that it can function independent of other political jurisdictions. Thus the electricity system should consist of a collection of micro grids, one per political jurisdiction, each of which is coupled to its neighbors via interties. A micro grid can be as large as the Canadian province of Ontario or as small as a college campus provided that all electricity rate and governance matters are decided by a single body within that microgrid. There should be enough self excited reserve generation within each jurisdiction that its micro grid is stable and can operate with any combination of its external interties disconnected.

Each micro grid needs its own regulatory authority which is responsible for affairs within that micro grid. The regulatory authority for each micro grid should set electricity rates within that micro grid, independent of legislated constraints. This regulatory authority must be responsible to jurisdiction politicians, but it is foolish for politicians to attempt to micro-manage the regulatory authority, especially with respect to electricity rate and technical matters. An example of the problems that politicians can cause is Ontario's Global Adjustment, which due to poorly thought legislation is applied to kWh instead of peak kW. The misapplication of the Global Adjustment discourages use of behind the meter energy storage, unnecessarily increases the blended retail electricity price per kWh and causes unnecessary use of fossil fuels.

Power transfers along interties must be mutually agreed to by all of the directly affected parties. Any party that experiences a power transfer along one of its interties that goes out of the specified tolerable range must have the right to disconnect that intertie without notice. This issue constrains wheeling of power between non-adjacent political jurisdictions.

A micro grid is phase synchronized to its neighbours via only one intertie. Other interties require either DC isolation or dedicated generation that is used to suppress loop currents between interties.

This grid architecture forces every jurisdiction to pay attention to generation reliability, stability and black start issues within that jurisdiction. If a particular jurisdiction becomes a problem to its neighbors, as indicated by excessive power flows along its interties, then its neighbors can isolate the offending jurisdiction until the offending jurisdiction gets its act together. Politicians must grasp that grid black start generally requires a significant fraction of large central coal, hydroelectric or nuclear generation. Electricity rate structures which make such large central plants financially insolvent are a risk to all electricity consumers who rely on reliable grid supplied electricity.

It is important to have a common national or international technical authority that can be used to resolve intertie related disputes because these matters are too technical for resolution via normal legal processes. To enable such resolution all intertie specifications should be expressed in a common technical language.

One of the consequences of this grid architecture is that all parties to an energy transfer along an intertie must be in agreement. This issue can potentially affect inter-state, inter-provincial and international commerce.

**Politicians ignore the issues of sufficiency of reliable generation and grid stability at their peril.** The issue of sufficiency of reliable generation is comparatively easy for non-technical persons to understand. However, the issue of grid stability is equally important but is far more complex to comprehend. In jurisdictions where there is a high penetration of wind and solar generation with AC line connected current source inverters electricity grid instability is already a serious problem.

**SUFFICIENCY OF RELIABLE GENERATION:**

If the generation within a micro grid cannot meet that micro grid's own load and its neighbors do not agree to supply additional energy when required then due to the law of conservation of energy that micro grid will have a blackout. One of the issues that all parties must face is the practical necessity for at least 15% surplus power generation capacity within each microgrid.

An issue that the parties must also face is that there is no free lunch. The fad for allowing intermittent renewable generation to run unconstrained into the electricity grid must stop. There are very real costs related to providing reliable generation when needed. The more unconstrained renewable generation that is connected the more the required grid balancing costs increase. Grid balancing via intertie power flows is not acceptable to non-consenting neighboring jurisdictions.

If wind and solar generation are contemplated the cost of the required balancing generation, energy storage and related transmission must also be met. The value of non-fossil electricity lies primarily in reliable capacity, not energy. This issue must be recognized in the governance of each micro grid. Failure to recognize this issue in electicity rates leads to low load factors which increase blended electricity costs per kWh.

To be reliable an intermittent renewable generator needs a very large battery or a large hydroelectric reservoir with connecting transmission. The cost per kW of that energy storage facility in combination with its related energy losses often far exceeds the cost per kW of a new nuclear power station.

A blunt reality is that the market value of intermittent renewable generation without sufficient balancing energy storage is only about $0.02 / kWh. There is a vast amount of misinformation relating to the costs of wind and solar energy as compared to the cost of reliable grid supplied energy. Often the grid supplied energy appears more expensive because part or all of the cost of capacity is included in the cost of grid energy per kWh. The only solution to this misinformation issue is to have separate charges to consumers for peak demand (kW or kVA) and energy (kWh) that reflect the actual or anticipated costs of capacity and energy. The sooner that regulatory bodies accept the necessity for these two separate charges, the better.

**GRID STABILITY:**

In addition to sufficiency of generation it is important to have grid stability in the presence of step changes in load. With mechanical synchronous generation grid stability is provided by the moment of inertia of the generation equipment's rotating mass. A self excited mechanical generator is usually controlled to provide a power output versus frequency with a slight negative slope (droop). In a multi-generator system usually only one large generator (the master generator) has frequency error integrating feedback which causes the system to achieve a line frequency of exactly 60 Hz. The other generators act as slave generators. Fixed output dispatched generation is used to follow major load changes. When the line frequency is exactly 60 Hz the generator voltage is set to the desired level via rotor field adjustment.

Today it is common practice to couple wind and solar generators to the grid using static power inverters. A voltage source dtatic power inverter can be designed to emulate a mechanical generator. However, the power output capacity of a voltage source static power inverter that can emulate a mechanical synchronous generator is about double the inverter's continuous full load output rating, which makes this type of power inverter expensive. A further issue with voltage source static power inverters is designing them so that power transients are proportionately shared over many such power inverters.

To avoid these cost issues renewable generators usually use current source power inverters. However, current source power inverters are unable to emulate mechanical moment of inertia and require other generation to set the grid voltage and grid frequency and to provide black start capability. Thus use of current source inverters makes the electricity grid less stable against step changes in load and make black start very difficult. A good rule of thumb is that at least 50% of the generation capacity in a micro grid must be self excited, must have stability equivalent to over damped synchronous mechanical generation and must be capable of stand alone black start.

A major problem with natural gas fuelled generation is gas line pressure. Most natural gas fuelled combustion turbines require a natural gas injection pressure of about 120 psig (9 bar absolute) to operate. If that natural gas pressure is derived from electrically driven compressors and there is a total electricity blackout the natural gas combustion turbines cannot start. Black start of the electricity grid relies on hydro-electric, coal and nuclear generation. As coal generation is phased out and nuclear generation is not replaced grid black start is an issue of increasing concern.

Black starting is generally best done using an electronic frequency and phase reference to bring each generator close to the desired frequency and phase before attempting to synchronize to the micro grid.

After a micro grid is operating as an isolated island that micro grid can be synchronized to its neighbors. A micro grid should not rely on an intertie to black start.

**TRANSIENT STEP RESPONSE:**

To understand grid response issues to step changes in load it is helpful to examine the power balance equation for a mechanical synchronous generator.

The kinetic energy Ek contained in the rotating moment of inertia I of the generator is:

Ek = (I W^2) / 2

where:

I = moment of inertia

and

W = shaft angular frequency

Hence differentiating with respect to time T gives:

dEk / dT = I W (dW / dT)

Assume a slave prime mover feedback control function of the form:

Ps = Po - Ka(W - Wo)

where:

Wo = shaft angular frequency setpoint

Ps = prime mover source power

Po = prime mover source power when W = Wo

Ka = feedback function constant

Then power balance on the generator shaft gives:

Ps = Pl + I W (dW / dT)

where:

Pl = load power

Note that when:

Ps = Pl

then:

dW / dT = 0

The generator shaft power balance equation gives:

Po - Ka(W - Wo) = Pl + I W (dW / dT)

**PRIOR STABLE CONDITION:**

At prior stable operating conditions:

Po = Plo

and

W = Wo

and

dW / dT = 0

**INITIAL CONDITION:**

Now assume that at T = To there is a step increase in load Pl from Plo to (Plo + D), where D is the amplitude of the power disturbance.

Since:

Po = Plo

the generator shaft power balance equation gives:

- Ka(W - Wo) = D + I W (dW / dT)

or

**W (dW / dT) + (Ka / I) (W - Wo) + [(D / I)] = 0**

At the instant when the step increase in load is applied:

**W = Wo**

giving:

Wo (dW / dT) + (D / I) = 0

or

**(dW / dT) = [- D / (I Wo)]**

**FINAL CONDITION:**

For a stable solution at T = Tf where:

T >> To:

**dW / dT = 0**

Recall that:

W (dW / dT) + (Ka / I) (W - Wo) + [(D / I)] = 0

implying that at T = Tf:

(Ka / I) (W - Wo) + [(D / I)] = 0

or

**(Wf - Wo) = - (D / Ka)**

where Wf is the final value of W.

Hence:

**Wf = Wo - (D / Ka)**

**FIND SOLUTION TO DIFFERENTIAL EQUATION:**

**W (dW / dT) + [(Ka / I) (W - Wo)] + [(D / I)] = 0**

that conforms to both the intial and final conditions.

Integrating the differential equation from T = To to T = T gives:

W^2 - Wo^2 + [Integral from T = To to T= T of:

{[(Ka / I) (W - Wo) dT] + [(D / I) dT}]} = 0

or

W^2 - Wo^2 + [Integral from T = To to T= T of:

{[(Ka / I) (W - Wo) dT] + [(Ka / I)(D / Ka) dT}]} = 0

or

W^2 - Wo^2 + [Integral from T = To to T= T of:

{(Ka / I) [W - Wo + (D / Ka)] dT}] = 0

Recall that:

Wf = Wo - (D / Ka)

Hence:

**W^2 - Wo^2 + [Integral from T = To to T= T of:
{(Ka / I) (W - Wf) dT}] = 0**

The shaft angular frequency W is related to the AC line frequency F by the equation:

**W = 2 Pi F / N**

where:

**N = 1 for a 3600 RPM generator;
N = 2 for a 1800 RPM generator;
N = 4 for a 900 RPM generator**

Similarly:

**Wo = 2 Pi Fo / N**

and

**Wf = 2 Pi Ff / N**

Hence the differential eequation becomes:

(2 Pi / N)^2 F^2 - (2 Pi / N)^2 Fo^2 + [Integral from T = To to T= T of {(Ka / I) ((2 Pi / N) F - (2 Pi / N) Ff) dT}] = 0

or

**F^2 - Fo^2 + [Integral from T = To to T= T of {(Ka N / 2 Pi I) ( F - Ff) dT}] = 0**

Define:

**G = (Ka N / 2 Pi I)**

which gives:

**F^2 - Fo^2 + [Integral from T = To to T= T of {G dT ( F - Ff)}] = 0**

In this equation:

T = time;

To = time at which a step change in load is applied;

Tf = value of T after disturbance has settled down;

F = AC line frequency as a function of time T;

Fo = (Wo N / 2 Pi) = AC line frequency setpoint;

Ff = Wf N / 2 Pi = line frequency after disturbance has settled down;

I = generator moment of inertia;

Po = prime mover power at T = To;

Pf = prime mover power at T = Tf;

Ka = feedback constant:

Ka = - (dPs / dW)

= - (dPs / dF) (dF / dW);

Recall that:

W = 2 Pi F / N

or

F = N W / 2 Pi

or

**dF / dW = N / 2 Pi**

**Assume a 100 kW generator**. To achieve reasonable frequency stability choose:

**(dPs / dF) = - (100 kW / 5 Hz)**

Thus:

**Ka** = - (dPs / dF) (dF / dW)

= (100 kW / 5 Hz) (N / 2 Pi)

= 10 N kW / Pi Hz

Choose:

**dT = (1 s / 60)**

Then:

G dT = (Ka N / 2 Pi I) dT

= [10 N kW/ Pi Hz] [N / 2 Pi I] [1 s / 60]

= [5 (N / Pi)^2 kW / Hz] [1 s / 60 I]

Express the differential equation in the form:

**F^2 = Fo^2 - [Integral from T = To to T = T of {G dT ( F - Ff)}]**

This differential equation can be numerically solved by iteration starting at F = Fo.

F^2 = Fo^2 - [Integral from T = To to T= T of {G dT (F - Ff)}]

F1^2 = Fo^2 - [G dT (Fo - Ff)]

F1 = {Fo^2 - [G dT (Fo - Ff)]}^0.5

(F2)^2 = Fo^2 - [G dT (Fo - Ff)] - [G dT (F1 - Ff)]

F2 = {Fo^2 - [G dT (Fo - Ff)] - [G dT (F1 - Ff)]}^0.5

In general:

**(Fn)^2 = {Fo^2 - Sum i = 0 to i = n-1 of [G dT (Fi - Ff)]}**

where:

Fo = Fo

and

**F(i+1) = {Fo^2 - Sum i = 0 to i = i of [G dT (Fi - Ff)]}^0.5**

If the system is insufficiently damped this relationship leads to frequency oscillations about F = Ff and power oscillations about P = Pf.

EXAMPLE - HEAVY OVER DAMPING:

Assume a moment of inertia of:

** I = (N^2 / Pi) kg m^2**

Assume a feedback control system that keeps the frequency in the range 57.5 Hz at full load to 62.5 Hz at no load. At T = To the load jumps from (1 / 2) load (50 kW at 60 Hz) to (3 / 4) load (75 kW at 58.75 Hz).

Fo = 60 Hz

Ff = 58.75 Hz

(2 Pi I) = 2 kg m^2

dT = (1 / 60) s

= - (dPs / dF) (dF / dW) (N / 2 Pi I) dT

= (100 kW / 5 Hz) (N / 2 Pi) (N / 2 Pi I)(1 s/ 60)

= (20 kW / Hz) (1 Hz s) (N^2 / 4 Pi^2)(1 s / 60) (1 / I)

= [(1000 W / kW)(1 kW / 12 Hz)(1 Hz s)(N^2 / Pi^2)(1 s / I)]

= 8.443446234 N^2 W s^2 / I

=

Then:

i | Fi | (Fi - Ff) | [G dT (Fi - Ff)] | Sum i = 0 to i = i of [G dT(Fi - Ff)] | {Fo^2 - Sum i = 0 to i = i of [G dT (Fi - Ff)]}^0.5 |
---|---|---|---|---|---|

0 | 60 Hz | 1.25 Hz | 33.1573 s^-2 | 33.1573 s^-2 | 59.7230 Hz |

1 | 59.7230 Hz | 0.97305 Hz | 25.81097 s^-2 | 58.9683 s^-2 | 59.5065 Hz |

2 | 59.5065 Hz | 0.756568 Hz | 20.06862 s^-2 | 79.0369 s^-2 | 59.3377 Hz |

3 | 59.3377 Hz | 0.5877 Hz | 15.5893 s^-2 | 94.6262 s^-2 | 59.2062 Hz |

4 | 59.2062 Hz | 0.4562 Hz | 12.1010 s^-2 | 106.7272 s^-2 | 59.1039 Hz |

5 | 59.1039 Hz | 0.3539 Hz | 9.3879 s^-2 | 116.1151 s^-2 | 59.0244 Hz |

6 | 59.0244 Hz | 0.27444 Hz | 7.2798 s^-2 | 123.3949 s^-2 | 58.9627 Hz |

7 | 58.9627 Hz | 0.2127 Hz | 5.6432 s^-2 | 129.0381 s^-2 | 58.9149 Hz |

8 | 58.9149 Hz | 0.1649 Hz | 4.3733 s^-2 | 133.4114 s^-2 | 58.8777 Hz |

9 | 58.8777 Hz | 0.1277 Hz | 3.3884 s^-2 | 136.7999 s^-2 | 58.84896 Hz |

10 | 58.84896 Hz | 0.09896 Hz | 2.6250 s^-2 | 139.4249 s^-2 | 58.8266 Hz |

11 | 58.8266 Hz | 0.07665 Hz | 2.0333 s^-2 | 141.4582 s^-2 | 58.8094 Hz |

12 | 58.8094 Hz | 0.05936 Hz | 1.5748 s^-2 | 143.0330 s^-2 | 58.7960 Hz |

12 X (1 s / 60) = (1 / 5) second

to give a

[(60 Hz - 58.796 Hz) / 1.25 Hz] X 100% = 96.32%

step response. However, if a power system has to accommodate a very high penetration of intermittent renewable generation using current source inverters this slow step response should be anticipated. It may be necessary to add additional spinning synchronous moment of inertia to an existing power system to stabilize it if there is a very high penetration of renewable generation. This amount of damping is also used in emergency power systems where ability to supply the inrush current related to on/off switching of elevators and fire pumps is more important than good frequency and power regulation.

EXAMPLE - OVER DAMPING:

Now try reducing I by a factor of 2 to:

**I = (N^2 / 2 Pi) kg m^2**

corresponding to:

**G dT = 53.0516925 / s**

i | Fi | (Fi - Ff) | [G dT (Fi - Ff)] | Sum i = 0 to i = i of [G dT (Fi - Ff)] | {Fo^2 - Sum i = 0 to i = i of [G dT (Fi - Ff)]}^0.5 |
---|---|---|---|---|---|

0 | 60 Hz | 1.25 Hz | 66.3146 s^-2 | 66.3146 s^-2 | 59.4448 Hz |

1 | 59.4448 Hz | 0.6948 Hz | 36.8603 s^-2 | 103.1749 s^-2 | 59.1340 Hz |

2 | 59.1340 Hz | 0.3840 Hz | 20.3697 s^-2 | 123.5446 s^-2 | 58.9615 Hz |

3 | 58.9615 Hz | 0.2115 Hz | 11.2191 s^-2 | 134.7637 s^-2 | 58.8663 Hz |

4 | 58.8663 Hz | 0.11626 Hz | 6.1677 s^-2 | 140.9314 s^-2 | 58.8138 Hz |

5 | 58.8138 Hz | 0.0638 Hz | 3.3872 s^-2 | 144.3186 s^-2 | 58.7850 Hz |

6 | 58.7850 Hz | 0.0350 Hz | 1.8591 s^-2 | 146.1777 s^-2 | 58.7692 Hz |

7 | 58.7692 Hz | 0.01923 Hz | 1.0201 s^-2 | 147.1978 s^-2 | 58.7605 Hz |

EXAMPLE - CRITICAL DAMPING:

Now try reducing I by a further factor of 2 to:

**I = (N^2 / 4 Pi) kg m^2**

corresponding to:

**G dT = 106.103385 / s**

giving:

i | Fi | (Fi - Ff) | [G dT (Fi - Ff)] | Sum i = 0 to i = i of [G dT (Fi - Ff)] | {Fo^2 - Sum i = 0 to i = i of [G dT (Fi - Ff)]}^0.5 |
---|---|---|---|---|---|

0 | 60 Hz | 1.25 Hz | 132.6292 s^-2 | 132.6292 s^-2 | 58.8844 Hz |

1 | 58.8844 Hz | 0.134384 Hz | 14.2586 s^-2 | 146.8878 s^-2 | 58.7632 Hz |

2 | 58.7632 Hz | 0.013187 Hz | 1.3992 s^-2 | 148.287 s^-2 | 58.7513 Hz |

3 | 58.7513 Hz | 0.00128 Hz | 0.1359 s^-2 | 148.4229 s^-2 | 58.7501 Hz |

EXAMPLE - UNDER DAMPING:

Now try reducing I by a further factor of 2 to
**I = (N^2 / 8 Pi) kg m^2**

corresponding to:

**G dT = 212.20677 / s**

giving:

i | Fi | (Fi - Ff) | [G (Fi - Ff)] | Sum i = 0 to i = i of [G (Fi - Ff)] | {Fo^2 - Sum i = 0 to i = i of [G (Fi - Ff)]}^0.5 |
---|---|---|---|---|---|

0 | 60 Hz | 1.25 Hz | 265.2585 s^-2 | 265.2585 s^-2 | 57.7472 Hz |

1 | 57.7472 Hz | - 1.00278 Hz | -212.7966 s^-2 | 52.4619 s^-2 | 59.5612 Hz |

2 | 59.5612 Hz | 0.81121 Hz | 172.1449 s^-2 | 224.6068 s^-2 | 58.0981 Hz |

3 | 58.0981 Hz | - 0.6519 Hz | - 138.3303 s^-2 | 86.2764 s^-2 | 59.2767 Hz |

4 | 59.2767 Hz | 0.5266 Hz | 111.7629 s^-2 | 198.0393 s^-2 | 58.3263 Hz |

5 | 58.3263 Hz | - 0.4237 Hz | - 89.9058 s^-2 | 108.1335 s^-2 | 59.0920 Hz |

6 | 59.0920 Hz | 0.3420 Hz | 72.5784 s^-2 | 180.7119 s^-2 | 58.47 Hz |

7 | 58.47 Hz | - 0.2753 Hz | - 58.4250 s^-2 | 122.2869 s^-2 | 58.9721 Hz |

8 | 58.9721 Hz | 0.2221 Hz | 47.1392 s^-2 | 169.4261 s^-2 | 58.5711 Hz |

9 | 58.5711 Hz | - 0.1789 Hz | -37.9635 s^-2 | 131.4626 s^-2 | 58.8943 Hz |

10 | 58.8943 Hz | 0.14429 Hz | 30.6194 s^-2 | 162.0820 s^-2 | 58.6337 Hz |

11 | 58.6337 Hz | -.11624 Hz | -24.6666 s^-2 | 137.4154 s^-2 | 58.8437 Hz |

12 | 58.8437 Hz | 0.0937 Hz | 19.8902 s^-2 | 157.3056 s^-2 | 58.6745 Hz |

**SUMMARY:**

The amplitude of the frequency change is set by the power disturbance D. The change in line frequncy F resulting from a step change in load power Pl of size D is expressed in terms of generation parameters I, N, Fo and feedback parameter Ka.

The moment of inertia I of the generator(s) plays an important role in damping potential frequency and power oscillation on the AC power grid that results from step changes in load. Each micro grid should have sufficient damping to attenuate both its own load disturbances and power disturbances that are imported from other grids via interties.

The above examples indicate that a 60 Hz power system with critical damping requires a moment of inertia at least:

**(10 N^2 / 4 Pi) kg m^2 / MW of synchronous generation**. If the system is to accommodate up to a 50% penetration of intermittent generation coupled using current source inverters the mechanical synchronous generation moment of inertia should be doubled to:

**(20 N^2 / 4 Pi) kg m^2 / MW of synchronous generation**.

An issue that is seldom adequately appreciated is that in practical two bearing generation equipment the flywheel weight and hence the moment of inertia is limited by the sustained load bearing capacity of the bearings. If voltage source inverters are used in place of synchronous generators the component ratings must be much larger than in comparable current source inverters.

**REVENUE GENERATION:**

A major issue with both retail electricity rates and compensating owners of non-fossil generation is that the value of non-fossil electricity lies primarily in reliable capacity rather than in energy.

Assume that over a year the projected load is a time dependent function of the form L(T), where L is measured in kW. Then generator i can potentially supply fraction Fi of the load by providing a net power capacity function of the form:

Pi(T) = 1.15 Fi L(T)

and energy:

E = Integral from T = January 1 to T = December 31 of:

Fi L(T) dT

If for any reason a generator cannot meet its power supply commitment that generator must meet its commitment via spot market electricity purchases.

A group of generators can form a consortium to bid on meeting the power requirement, but the consortim members must all be proportionately liable for meeting the commitment.

The successful generators can earn extra revenue by selling additional firm energy and interruptible energy.

The maximum possible additional firm energy per annum is:

[Sum of (monthly power capacity bids) 730.5 hours] - E

Generators should be paid monthly for meeting their contracted capacity, for supplying their contracted energy, for supplying additonal firm energy and for supplying extra interruptible energy. A generator might earn extra revenue by providing spot market power and spot market energy to meet shortfalls by other generators. A generator may also be paid a premium if it has capacity to support grid black start.

A generator bids to supply a minimum specified capacity for each month for 12 successive months. A generator that fails to meet its capacity bid must pay for replacement capacity purchased at the spot market price. The generator's capacity bid implicitly includes 15% extra capacity. The capacity bid implies availability of at least:

1.15 (730.5 kWh) = 840.075 kWh

of firm energy per bid capacity kW. The generator might be able to sell unpurchased kWh into the interruptible kWh market. If another generator fails to meet its commitments the generator might also be able to sell spot market capacity and energy. Note that in the annual peak month the cost of spot market capacity heads toward infinity.

The capacity that can be bid by an intermittent generator is generally limited by that generator's reliable energy storage capacity.

Most wind and solar generators will have energy outputs that far exceed their firm capacity ratings. This extra energy must either be constrained or sold in a local distribution market that does not require use of the public transmission grid.

Typically the revenue of a reliable generator is about:

** [($50 / kW) + ($0.01 / kWh)]**.

However, absent behind the meter energy storage and an interruptible energy market a generator may only be able to sell:

(350 kWh / month) / kW

of bid monthly power capacity.

If a generator fails to meet its capacity bid it must pay for replacement capacity. The cost of that replacement capacity may be as much as 20X the normal value of the missing capacity. Hence intermittent generators must have a extremely high certainty about their energy supply and energy storage before bidding into the capacity market. Another way to view this situation is that absent sufficient energy storage the value of intermittent generation is limited to the value of the fossil fuels that it can displace.

This web page last updated August 10, 2018.

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