SlideShare uma empresa Scribd logo
1 de 29
Baixar para ler offline
Economic Load Dispatch
I The idea is to minimize the cost of electricity generation
without sacrificing quality and reliability.
I Therefore, the production cost is minimized by operating
plants economically.
I Since the load demand varies, the power generation must vary
accordingly to maintain the power balance.
I The turbine-governor must be controlled such that the
demand is met economically.
I This arises when there are multiple choices.
Economic Distribution of Loads between the units in a Plant:
I To determine the economic distribution of load between
various generating units, the variable operating costs of the
units must be expressed in terms of the power output.
I Fuel cost is the principle factor in thermal and nuclear power
plants. It must be expressed in terms of the power output.
I Operation and Maintenance costs can also be expressed in
terms of the power output.
I Fixed costs, such as the capital cost, depreciation etc., are not
included in the fuel cost.
Let us define the input cost of an unit i ,Fi in Rs./h and the power
output of the unit as Pi . Then the input cost can be expressed in
terms of the power output as
Fi = ai P2
i + bi Pi + ci Rs/h
Where ai , bi and ci are fuel cost coefficients.
The incremental operating cost of each unit is
λi =
dFi
dPi
= 2ai Pi + bi Rs./MWh
Let us assume that there ar N units in a plant.
1
N
PD
The total fuel cost is
FT = F1 + F2 + · · · + FN =
N
X
i=1
Fi Rs./h
All the units have to supply a load demand of PD MW.
P1 + P2 + · · · + PN = PD
N
X
i=1
Pi = PD
min FT =
N
X
i=1
Fi
Subject to
N
X
i=1
Pi = PD
It is a constrained optimization problem. Let us form the
Lagrangian function.
L = FT + λ(PD −
N
X
i=1
Pi )
To find the optimum,
∂L
∂Pi
= 0 i = 1, 2, · · · , N
∂L
∂λ
= 0
dFi
dPi
= λ i = 1, 2, · · · , N
N
X
i=1
Pi = PD
N + 1 linear equations need to be solved for N + 1 variables.
For economical division of load between units within a plant, the
criterion is that all units must operate at the same incremental fuel
cost.
dF1
dP1
=
dF2
dP2
= · · · =
dFn
dPn
= λ
This is called the coordination equation.
P1 (MW)
dF
1
dP
1
(Rs/MWhr)
P2 (MW)
dF
2
dP
2
(Rs/MWhr)
λ∗
P∗
2
P∗
1
Example : Consider two units of a plant that have fuel costs of
F1 = 0.2P2
1 + 40P1 + 120 Rs./h
F2 = 0.25P2
2 + 30P2 + 150 Rs./h
1. Determine the economic operating schedule and the
corresponding cost of generation for the demand of 180 MW.
2. If the load is equally shared by both the units, determine the
savings obtained by loading the units optimally.
1. For economical dispatch,
dF1
dP1
=
dF2
dP2
0.4P1 + 40 = 0.5P2 + 30
and
P1 + P2 = 180
On solving the above two equations,
P1 = 88.89 MW; P2 = 91.11 MW
The cost of generation is
FT = F1 + F2 = 10, 214.43 Rs./h
2. If the load is shared equally,
P1 = 90 MW; P2 = 90 MW
The cost of generation is
FT = 10, 215 Rs./h
Therefore, the saving will be 0.57 Rs./h
Generator Limits:
The power generation limit of each unit is given by the inequality
constraints
Pi,min ≀ Pi ≀ Pi,max i = 1, · · · , N
I The maximum limit Pmax is the upper limit of power
generation capacity of each unit.
I Whereas, the lower limit Pmin pertains to the thermal
consideration of operating a boiler in a thermal or nuclear
generating station.
How to consider the limits
I If any one of the optimal values violates its limits, fix the
generation of that unit to the violated value.
I Optimally dispatch the reduced load among the remaining
generators.
Example: The fuel cost functions for three thermal plants are
F1 = 0.4P2
1 + 10P1 + 25 Rs./h
F2 = 0.35P2
2 + 5P2 + 20 Rs./h
F3 = 0.475P2
3 + 15P3 + 35 Rs./h
The generation limits of the units are
30 MW ≀ P1 ≀ 500 MW
30 MW ≀ P2 ≀ 500 MW
30 MW ≀ P3 ≀ 250 MW
Find the optimum schedule for the load of 1000 MW.
For optimum dispatch,
dF1
dP1
=
dF2
dP2
=
dF3
dP3
0.8P1 + 10 = 0.7P2 + 5
0.7P2 + 5 = 0.9P3 + 15
and
P1 + P2 + P3 = 1000
On solving the above three equations,
P1 = 334.3829 MW; P2 = 389.2947 MW; P3 = 276.3224 MW
Since the unit 3 violates its maximum limit,
P3 = 250 MW
The remaining load (750 MW) is scheduled optimally among 1 and
2 units.
0.8P1 + 10 = 0.7P2 + 5
P1 + P2 = 750
On solving the above equations,
P1 = 346.6667 MW; P2 = 403.3333 MW
Therefore, the final load distribution is
P1 = 346.6667 MW; P2 = 403.3333 MW; P3 = 250 MW
Economic Distribution of Loads between different Plants:
I If the plants are spread out geographically, line losses must be
considered.
I The line losses are expressed as a function of generator
outputs.
min FT =
N
X
i=1
Fi
Subject to
N
X
i=1
Pi = PL + PD
where PL = f (Pi ). It is a nonlinear function of Pi . Let us form the
Lagrangian function.
L = FT + λ(PD + PL −
N
X
i=1
Pi )
To find the optimum,
∂L
∂Pi
= 0 i = 1, 2, · · · , N
∂L
∂λ
= 0
dFi
dPi
+ λ
∂PL
∂Pi
= λ i = 1, 2, · · · , N
dFi
dPi
= λ

1 −
∂PL
∂Pi

1
1 −
∂PL
∂Pi
dFi
dPi
= λ
Let us define the penalty factor Li for ith generator.
Li
dFi
dPi
= λ
where Li =
1
1 −
∂PL
∂Pi
.
For economical division of load between plants, the criterion is
L1
dF1
dP1
= L2
dF2
dP2
= · · · = Ln
dFn
dPn
= λ
This is called the exact coordination equation.
Since PL is a nonlinear function of Pi , the following N + 1
equations need to be solved numerically for N + 1 variables.
Li
dFi
dPi
= λ i = 1, 2, · · · , N
N
X
i=1
Pi = PL + PD
The transmission losses are usually expressed as
PL = PT
BP
where P = [P1, P2, · · · Pn] and B is a symmetric matrix given by
B =
ïŁź
ïŁŻ
ïŁŻ
ïŁŻ
ïŁ°
B11 B12 · · · B1n
B21 B22 · · · B2n
.
.
.
.
.
.
...
.
.
.
Bn1 Bn2 · · · Bnn
ïŁč
ïŁș
ïŁș
ïŁș
ïŁ»
The elements of the matrix B are called the loss coefficients.
Example: Consider a two bus system.
1
O 2
O
Load
P1 P2
The incremental fuel cost characteristics of plant 1 and plant 2 are
given by
dF1
dP1
= 0.025P1 + 14 Rs/MWHr
dF2
dP2
= 0.05P2 + 16 Rs/MWHr
If 200 MW of power is transmitted from plant 1 to the load, a
transmission loss of 20 MW will be incurred. Find the optimum
generation schedule and the cost of received power for a load
demand of 204.41 MW.
PL =

P1 P2


B11 B12
B21 B22
 
P1
P2

Since the load is at bus 2, P2 will not have any effect on PL.
B12 = B21 = 0; B22 = 0
Therefore,
PL = B11P2
1
For 200 MW of P1, PL = 20 MW.
20 = B112002
B11 = 0.0005 MW−1
PL = 0.0005P2
1
For optimum dispatch,
L1
dF1
dP1
= L2
dF2
dP2
= λ
Since PL is a function of P1 alone,
L1 =
1
1 −
∂PL
∂P1
=
1
1 − 0.001P1
L2 = 1

1
1 − 0.001P1

0.025P1 + 14 = 0.05P2 + 16
On simplification,
0.041P1 − 0.05P2 + 0.00005P1P2 = 2
and
P1 + P2 − 0.0005P2
1 = 204.41
f1(P1, P2) = 2
f2(P1, P2) = 204.41
Let us solve them by N-R method.
∆f = J∆P
where
∆f =

2 − f1(P1, P2)
204.41 − f2(P1, P2)

J =
ïŁź
ïŁŻ
ïŁ°
∂f1
∂P1
∂f1
∂P2
∂f2
∂P1
∂f2
∂P2
ïŁč
ïŁș
ïŁ»
To find the initial estimate : Let us solve the problem with out loss.
0.025P1 + 14 = 0.05P2 + 16
P1 + P2 = 204.41
P0
1 = 162.94; P0
2 = 41.47
First Iteration :
∆f0
=

2 − f1(P0
1 , P0
2 )
204.41 − f2(P0
1 , P0
2 )

=

−2.9449
13.2747

J0
=

0.0431 −0.0419
0.8371 0.9585


∆P0
1
∆P0
2

=

−29.7060
39.7906


P1
1
P1
2

=

P0
1
P0
2

+

∆P0
1
∆P0
2

=

133.2340
81.2606
It took 6 iterations to converge.
P1 = 133.3153 MW P2 = 79.9812 MW
The cost of received power is
λ = L2
dF2
dP2
= 1 × (0.05 × 79.9812 + 16) = 19.9991 Rs./MWh
λ-iteration Method
PL =
N
X
i=1
N
X
j=1
Pi Bij Pj
The exact coordination equation is
dFi
dPi
+ λ
∂PL
∂Pi
= λ
It can be written as
2ai Pi + bi + 2λ
N
X
j=1
Bij Pj = λ
2ai Pi + bi + 2λBii Pi + 2λ
N
X
j=1
j6=i
Bij Pj = λ
Pi =
λ − bi − 2λ
PN
j=1
j6=i
Bij Pj
2(ai + λBii )
On substituting this in the power balance equation,
N
X
i=1
Pi = PD + PL
N
X
i=1
λ − bi − 2λ
PN
j=1
j6=i
Bij Pj
2(ai + λBii )
= PD + PL
f (λ) = PD + PL
This needs to be solved repeatedly for different values of λ.
Expanding it using Taylor’s series about an initial point (λ0) and
neglecting the higher order terms.
f (λ0
) + (
df (λ)
dλ
)0
∆λ0
≈ PD + P0
L
∆λ0
=
PD + P0
L − f (λ0)
(df (λ)
dλ )0
where
f (λ0
) =
N
X
i=1
P0
i
(
df (λ)
dλ
)0
=
N
X
i=1
(
dPi
dλ
)0
=
N
X
i=1
ïŁ«
ïŁŹ
ïŁ­
ai + bi Bii − 2ai
PN
j=1
j6=i
Bij P0
j
2(ai + λ0Bii )2
ïŁ¶
ïŁ·
ïŁž
Therefore,
λ1
= λ0
+ ∆λ0
In general,
λk+1
= λk
+ ∆λk
where
∆λk
=
PD + Pk
L −
PN
i=1 Pk
i
PN
i=1
ïŁ«
ïŁ­
ai +bi Bii −2ai
PN
j=1
j6=i
Bij Pk
j
2(ai +λk Bii )2
ïŁ¶
ïŁž
I Start with λk.
I Find Pk
i as follows:
Pk
i =
λk − bi − 2λk
PN
j=1
j6=i
Bij Pk
j
2(ai + λkBii )
I Find Pk
L using the following equation.
Pk
L =
N
X
i=1
N
X
j=1
Pk
i Bij Pk
j
I Repeat the above steps till |PD + Pk
L −
PN
i=1 Pk
i | ≀ .
I To start with, assume λ0 such that it is greater than the
largest value of the coefficients b.
Example : Let us take the same example. The incremental fuel
cost characteristics of plant 1 and plant 2 are given by
dF1
dP1
= 0.025P1 + 14 Rs/MWHr
dF2
dP2
= 0.05P2 + 16 Rs/MWHr
PL = 0.0005P2
1
1. Assume λ0 = 17.
2. P0
1 and P0
2 are
P0
1 =
λ0 − b1
2(a1 + λ0B11)
= 71.4286 MW
P0
2 =
λ0 − b2
2(a2)
= 20 MW
3. It took 8 iterations to converge.
λ = 19.9991 Rs/MWhr P1 = 133.3152 MW P2 = 79.9812 MW

Mais conteĂșdo relacionado

Mais procurados

Resistance,bundled conductor,skin effect,proximity effect
Resistance,bundled conductor,skin effect,proximity effectResistance,bundled conductor,skin effect,proximity effect
Resistance,bundled conductor,skin effect,proximity effectvishalgohel12195
 
IP protection or ingress protection
IP protection or ingress protectionIP protection or ingress protection
IP protection or ingress protectionKamran Hassan
 
over head insulators
over head insulatorsover head insulators
over head insulatorsFahad Rasheed
 
Protection settings calculation
Protection settings calculationProtection settings calculation
Protection settings calculationLANOGWA RODGERS
 
Electrical substations: 132 KV
Electrical substations: 132 KV Electrical substations: 132 KV
Electrical substations: 132 KV Girish Gupta
 
SAG-TENSION CALCULATION METHODS FOR OVERHEAD LINES
SAG-TENSION CALCULATION METHODS FOR OVERHEAD LINESSAG-TENSION CALCULATION METHODS FOR OVERHEAD LINES
SAG-TENSION CALCULATION METHODS FOR OVERHEAD LINESPower System Operation
 
4. Generator Step Up Transformer
4. Generator Step Up Transformer4. Generator Step Up Transformer
4. Generator Step Up TransformerChinedu Isiadinso
 
Power cables
Power cablesPower cables
Power cablescollege
 
Design of substation (with Transformer Design)
Design of substation (with Transformer Design) Design of substation (with Transformer Design)
Design of substation (with Transformer Design) SayanSarkar55
 
Understanding transformer vector group
Understanding transformer vector groupUnderstanding transformer vector group
Understanding transformer vector groupShyamkant Vasekar
 
Voltage Drop Calculation.pdf
Voltage Drop Calculation.pdfVoltage Drop Calculation.pdf
Voltage Drop Calculation.pdfMesiasJohnFederico
 
Cable sizing to withstand short circuit current
Cable sizing to withstand short circuit currentCable sizing to withstand short circuit current
Cable sizing to withstand short circuit currentLeonardo ENERGY
 
Electrical Engineering (EE) presentation on POWER CABLES
Electrical Engineering (EE) presentation on POWER CABLESElectrical Engineering (EE) presentation on POWER CABLES
Electrical Engineering (EE) presentation on POWER CABLESPritish Parihar
 

Mais procurados (20)

Gas insulated substation.
Gas insulated substation.Gas insulated substation.
Gas insulated substation.
 
ECNG 3013 A
ECNG 3013 AECNG 3013 A
ECNG 3013 A
 
Resistance,bundled conductor,skin effect,proximity effect
Resistance,bundled conductor,skin effect,proximity effectResistance,bundled conductor,skin effect,proximity effect
Resistance,bundled conductor,skin effect,proximity effect
 
IP protection or ingress protection
IP protection or ingress protectionIP protection or ingress protection
IP protection or ingress protection
 
Ppt super
Ppt superPpt super
Ppt super
 
over head insulators
over head insulatorsover head insulators
over head insulators
 
Ppt
PptPpt
Ppt
 
Protection settings calculation
Protection settings calculationProtection settings calculation
Protection settings calculation
 
Electrical substations: 132 KV
Electrical substations: 132 KV Electrical substations: 132 KV
Electrical substations: 132 KV
 
SAG-TENSION CALCULATION METHODS FOR OVERHEAD LINES
SAG-TENSION CALCULATION METHODS FOR OVERHEAD LINESSAG-TENSION CALCULATION METHODS FOR OVERHEAD LINES
SAG-TENSION CALCULATION METHODS FOR OVERHEAD LINES
 
4. Generator Step Up Transformer
4. Generator Step Up Transformer4. Generator Step Up Transformer
4. Generator Step Up Transformer
 
Power cables
Power cablesPower cables
Power cables
 
Design of substation (with Transformer Design)
Design of substation (with Transformer Design) Design of substation (with Transformer Design)
Design of substation (with Transformer Design)
 
Understanding transformer vector group
Understanding transformer vector groupUnderstanding transformer vector group
Understanding transformer vector group
 
Power factor
Power factorPower factor
Power factor
 
Voltage Drop Calculation.pdf
Voltage Drop Calculation.pdfVoltage Drop Calculation.pdf
Voltage Drop Calculation.pdf
 
Aerial cables
Aerial cablesAerial cables
Aerial cables
 
Cable sizing to withstand short circuit current
Cable sizing to withstand short circuit currentCable sizing to withstand short circuit current
Cable sizing to withstand short circuit current
 
Xlpe insulated cables
Xlpe insulated cablesXlpe insulated cables
Xlpe insulated cables
 
Electrical Engineering (EE) presentation on POWER CABLES
Electrical Engineering (EE) presentation on POWER CABLESElectrical Engineering (EE) presentation on POWER CABLES
Electrical Engineering (EE) presentation on POWER CABLES
 

Semelhante a Economic_Load_Dispatch.pdf

Project on economic load dispatch
Project on economic load dispatchProject on economic load dispatch
Project on economic load dispatchayantudu
 
economic load dispatch and unit commitment power_system_operation.pdf
economic load dispatch and unit commitment power_system_operation.pdfeconomic load dispatch and unit commitment power_system_operation.pdf
economic load dispatch and unit commitment power_system_operation.pdfArnabChakraborty499766
 
An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...
An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...
An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...IOSR Journals
 
211658558-Chapter-4-Economic-Dispatch.pdf
211658558-Chapter-4-Economic-Dispatch.pdf211658558-Chapter-4-Economic-Dispatch.pdf
211658558-Chapter-4-Economic-Dispatch.pdfyoziscijunior
 
Ece4762011 lect16
Ece4762011 lect16Ece4762011 lect16
Ece4762011 lect16miguelmena2013
 
Mr. Bakar Presentation for group discussion.docx
Mr. Bakar Presentation for group discussion.docxMr. Bakar Presentation for group discussion.docx
Mr. Bakar Presentation for group discussion.docxCyberMohdSalahShoty
 
Chapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptx
Chapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptxChapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptx
Chapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptxkyawmyint19
 
Economic Load Dispatch.ppt
Economic Load Dispatch.pptEconomic Load Dispatch.ppt
Economic Load Dispatch.pptSuraj Dhungel
 
3 Economic Dispatch Of Thermal
3 Economic Dispatch Of Thermal3 Economic Dispatch Of Thermal
3 Economic Dispatch Of ThermalKimberly Pulley
 
ECE476_2016_Lect17.pptx
ECE476_2016_Lect17.pptxECE476_2016_Lect17.pptx
ECE476_2016_Lect17.pptxFeehaAreej
 
Aircraft propulsion non ideal turbofan cycle analysis
Aircraft propulsion   non ideal turbofan cycle analysisAircraft propulsion   non ideal turbofan cycle analysis
Aircraft propulsion non ideal turbofan cycle analysisAnurak Atthasit
 
An Algorithm For The Combined Distribution And Assignment Problem
An Algorithm For The Combined Distribution And Assignment ProblemAn Algorithm For The Combined Distribution And Assignment Problem
An Algorithm For The Combined Distribution And Assignment ProblemAndrew Parish
 
11.determination of spot price and optimal power flow in
11.determination of spot price and optimal power flow in11.determination of spot price and optimal power flow in
11.determination of spot price and optimal power flow inAlexander Decker
 
Determination of spot price and optimal power flow in
Determination of spot price and optimal power flow inDetermination of spot price and optimal power flow in
Determination of spot price and optimal power flow inAlexander Decker
 
Thermodynamics (2013 new edition) copy
Thermodynamics (2013 new edition)   copyThermodynamics (2013 new edition)   copy
Thermodynamics (2013 new edition) copyYuri Melliza
 
Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...
Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...
Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...Catherine Maria Centanaro Chavez
 
Lecture 16
Lecture 16Lecture 16
Lecture 16Forward2025
 

Semelhante a Economic_Load_Dispatch.pdf (20)

Project on economic load dispatch
Project on economic load dispatchProject on economic load dispatch
Project on economic load dispatch
 
economic load dispatch and unit commitment power_system_operation.pdf
economic load dispatch and unit commitment power_system_operation.pdfeconomic load dispatch and unit commitment power_system_operation.pdf
economic load dispatch and unit commitment power_system_operation.pdf
 
An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...
An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...
An Application Jeevan – Kushalaiah Method to Find Lagrangian Multiplier in Ec...
 
211658558-Chapter-4-Economic-Dispatch.pdf
211658558-Chapter-4-Economic-Dispatch.pdf211658558-Chapter-4-Economic-Dispatch.pdf
211658558-Chapter-4-Economic-Dispatch.pdf
 
Ece4762011 lect16
Ece4762011 lect16Ece4762011 lect16
Ece4762011 lect16
 
Mr. Bakar Presentation for group discussion.docx
Mr. Bakar Presentation for group discussion.docxMr. Bakar Presentation for group discussion.docx
Mr. Bakar Presentation for group discussion.docx
 
Chapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptx
Chapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptxChapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptx
Chapter 4 Dr. Khin Thuzar Soe Economic Operation of power System - Copy.pptx
 
Economic Load Dispatch.ppt
Economic Load Dispatch.pptEconomic Load Dispatch.ppt
Economic Load Dispatch.ppt
 
3 Economic Dispatch Of Thermal
3 Economic Dispatch Of Thermal3 Economic Dispatch Of Thermal
3 Economic Dispatch Of Thermal
 
ECE4762011_Lect16.ppt
ECE4762011_Lect16.pptECE4762011_Lect16.ppt
ECE4762011_Lect16.ppt
 
ECE476_2016_Lect17.pptx
ECE476_2016_Lect17.pptxECE476_2016_Lect17.pptx
ECE476_2016_Lect17.pptx
 
Economic Dispatch
Economic DispatchEconomic Dispatch
Economic Dispatch
 
Aircraft propulsion non ideal turbofan cycle analysis
Aircraft propulsion   non ideal turbofan cycle analysisAircraft propulsion   non ideal turbofan cycle analysis
Aircraft propulsion non ideal turbofan cycle analysis
 
An Algorithm For The Combined Distribution And Assignment Problem
An Algorithm For The Combined Distribution And Assignment ProblemAn Algorithm For The Combined Distribution And Assignment Problem
An Algorithm For The Combined Distribution And Assignment Problem
 
11.determination of spot price and optimal power flow in
11.determination of spot price and optimal power flow in11.determination of spot price and optimal power flow in
11.determination of spot price and optimal power flow in
 
Determination of spot price and optimal power flow in
Determination of spot price and optimal power flow inDetermination of spot price and optimal power flow in
Determination of spot price and optimal power flow in
 
Thermodynamics (2013 new edition) copy
Thermodynamics (2013 new edition)   copyThermodynamics (2013 new edition)   copy
Thermodynamics (2013 new edition) copy
 
F ch
F chF ch
F ch
 
Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...
Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...
Solucionario IntroducciĂłn a la Termodinamica en IngenierĂ­a QuĂ­mica: Smith, Va...
 
Lecture 16
Lecture 16Lecture 16
Lecture 16
 

Mais de LucasMogaka

1502957399lectrure_5_KUET.pptx
1502957399lectrure_5_KUET.pptx1502957399lectrure_5_KUET.pptx
1502957399lectrure_5_KUET.pptxLucasMogaka
 
Ch08_PPT_Fund_Elec_Circ_5e.ppt
Ch08_PPT_Fund_Elec_Circ_5e.pptCh08_PPT_Fund_Elec_Circ_5e.ppt
Ch08_PPT_Fund_Elec_Circ_5e.pptLucasMogaka
 
Power_plant_ecomices.pptx
Power_plant_ecomices.pptxPower_plant_ecomices.pptx
Power_plant_ecomices.pptxLucasMogaka
 
Transmission_and_Distribution_System.pptx
Transmission_and_Distribution_System.pptxTransmission_and_Distribution_System.pptx
Transmission_and_Distribution_System.pptxLucasMogaka
 
Basic_Laws.ppt
Basic_Laws.pptBasic_Laws.ppt
Basic_Laws.pptLucasMogaka
 
loadforecasting-190205135237.pptx
loadforecasting-190205135237.pptxloadforecasting-190205135237.pptx
loadforecasting-190205135237.pptxLucasMogaka
 
NR-Power Flow.pdf
NR-Power Flow.pdfNR-Power Flow.pdf
NR-Power Flow.pdfLucasMogaka
 
Section 5 Power Flow.pdf
Section 5 Power Flow.pdfSection 5 Power Flow.pdf
Section 5 Power Flow.pdfLucasMogaka
 
Ac_steady_state_analyis.pptx
Ac_steady_state_analyis.pptxAc_steady_state_analyis.pptx
Ac_steady_state_analyis.pptxLucasMogaka
 
slides_12_ch 14-2- complex numbers.pdf
slides_12_ch 14-2- complex numbers.pdfslides_12_ch 14-2- complex numbers.pdf
slides_12_ch 14-2- complex numbers.pdfLucasMogaka
 
MATLAB DEKUT 2019.doc
MATLAB DEKUT 2019.docMATLAB DEKUT 2019.doc
MATLAB DEKUT 2019.docLucasMogaka
 
LOAD FORECASTING.ppt
LOAD FORECASTING.pptLOAD FORECASTING.ppt
LOAD FORECASTING.pptLucasMogaka
 
0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdf
0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdf0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdf
0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdfLucasMogaka
 
18053522.pdf
18053522.pdf18053522.pdf
18053522.pdfLucasMogaka
 
CiT-03.pptx
CiT-03.pptxCiT-03.pptx
CiT-03.pptxLucasMogaka
 
CiT-02.pptx
CiT-02.pptxCiT-02.pptx
CiT-02.pptxLucasMogaka
 
Ac_steady_state_analyis.pptx
Ac_steady_state_analyis.pptxAc_steady_state_analyis.pptx
Ac_steady_state_analyis.pptxLucasMogaka
 
CiT-03.pptx
CiT-03.pptxCiT-03.pptx
CiT-03.pptxLucasMogaka
 
1340050227.pdf
1340050227.pdf1340050227.pdf
1340050227.pdfLucasMogaka
 
EE-8353 EDC COURSE MATERIAL.pdf
EE-8353 EDC COURSE MATERIAL.pdfEE-8353 EDC COURSE MATERIAL.pdf
EE-8353 EDC COURSE MATERIAL.pdfLucasMogaka
 

Mais de LucasMogaka (20)

1502957399lectrure_5_KUET.pptx
1502957399lectrure_5_KUET.pptx1502957399lectrure_5_KUET.pptx
1502957399lectrure_5_KUET.pptx
 
Ch08_PPT_Fund_Elec_Circ_5e.ppt
Ch08_PPT_Fund_Elec_Circ_5e.pptCh08_PPT_Fund_Elec_Circ_5e.ppt
Ch08_PPT_Fund_Elec_Circ_5e.ppt
 
Power_plant_ecomices.pptx
Power_plant_ecomices.pptxPower_plant_ecomices.pptx
Power_plant_ecomices.pptx
 
Transmission_and_Distribution_System.pptx
Transmission_and_Distribution_System.pptxTransmission_and_Distribution_System.pptx
Transmission_and_Distribution_System.pptx
 
Basic_Laws.ppt
Basic_Laws.pptBasic_Laws.ppt
Basic_Laws.ppt
 
loadforecasting-190205135237.pptx
loadforecasting-190205135237.pptxloadforecasting-190205135237.pptx
loadforecasting-190205135237.pptx
 
NR-Power Flow.pdf
NR-Power Flow.pdfNR-Power Flow.pdf
NR-Power Flow.pdf
 
Section 5 Power Flow.pdf
Section 5 Power Flow.pdfSection 5 Power Flow.pdf
Section 5 Power Flow.pdf
 
Ac_steady_state_analyis.pptx
Ac_steady_state_analyis.pptxAc_steady_state_analyis.pptx
Ac_steady_state_analyis.pptx
 
slides_12_ch 14-2- complex numbers.pdf
slides_12_ch 14-2- complex numbers.pdfslides_12_ch 14-2- complex numbers.pdf
slides_12_ch 14-2- complex numbers.pdf
 
MATLAB DEKUT 2019.doc
MATLAB DEKUT 2019.docMATLAB DEKUT 2019.doc
MATLAB DEKUT 2019.doc
 
LOAD FORECASTING.ppt
LOAD FORECASTING.pptLOAD FORECASTING.ppt
LOAD FORECASTING.ppt
 
0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdf
0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdf0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdf
0ea1cdf161957c644e8c0b524c973c7e7b2c - Copy.pdf
 
18053522.pdf
18053522.pdf18053522.pdf
18053522.pdf
 
CiT-03.pptx
CiT-03.pptxCiT-03.pptx
CiT-03.pptx
 
CiT-02.pptx
CiT-02.pptxCiT-02.pptx
CiT-02.pptx
 
Ac_steady_state_analyis.pptx
Ac_steady_state_analyis.pptxAc_steady_state_analyis.pptx
Ac_steady_state_analyis.pptx
 
CiT-03.pptx
CiT-03.pptxCiT-03.pptx
CiT-03.pptx
 
1340050227.pdf
1340050227.pdf1340050227.pdf
1340050227.pdf
 
EE-8353 EDC COURSE MATERIAL.pdf
EE-8353 EDC COURSE MATERIAL.pdfEE-8353 EDC COURSE MATERIAL.pdf
EE-8353 EDC COURSE MATERIAL.pdf
 

Último

Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar â‰ŒđŸ” Delhi door step de...
Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar  â‰ŒđŸ” Delhi door step de...Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar  â‰ŒđŸ” Delhi door step de...
Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar â‰ŒđŸ” Delhi door step de...9953056974 Low Rate Call Girls In Saket, Delhi NCR
 
Extrusion Processes and Their Limitations
Extrusion Processes and Their LimitationsExtrusion Processes and Their Limitations
Extrusion Processes and Their Limitations120cr0395
 
data_management_and _data_science_cheat_sheet.pdf
data_management_and _data_science_cheat_sheet.pdfdata_management_and _data_science_cheat_sheet.pdf
data_management_and _data_science_cheat_sheet.pdfJiananWang21
 
Online banking management system project.pdf
Online banking management system project.pdfOnline banking management system project.pdf
Online banking management system project.pdfKamal Acharya
 
UNIT - IV - Air Compressors and its Performance
UNIT - IV - Air Compressors and its PerformanceUNIT - IV - Air Compressors and its Performance
UNIT - IV - Air Compressors and its Performancesivaprakash250
 
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...ranjana rawat
 
UNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICS
UNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICSUNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICS
UNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICSrknatarajan
 
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELLPVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELLManishPatel169454
 
Booking open Available Pune Call Girls Koregaon Park 6297143586 Call Hot Ind...
Booking open Available Pune Call Girls Koregaon Park  6297143586 Call Hot Ind...Booking open Available Pune Call Girls Koregaon Park  6297143586 Call Hot Ind...
Booking open Available Pune Call Girls Koregaon Park 6297143586 Call Hot Ind...Call Girls in Nagpur High Profile
 
Coefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptxCoefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptxAsutosh Ranjan
 
Generative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPTGenerative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPTbhaskargani46
 
University management System project report..pdf
University management System project report..pdfUniversity management System project report..pdf
University management System project report..pdfKamal Acharya
 
BSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptx
BSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptxBSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptx
BSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptxfenichawla
 
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Bookingdharasingh5698
 
Intze Overhead Water Tank Design by Working Stress - IS Method.pdf
Intze Overhead Water Tank  Design by Working Stress - IS Method.pdfIntze Overhead Water Tank  Design by Working Stress - IS Method.pdf
Intze Overhead Water Tank Design by Working Stress - IS Method.pdfSuman Jyoti
 
UNIT-III FMM. DIMENSIONAL ANALYSIS
UNIT-III FMM.        DIMENSIONAL ANALYSISUNIT-III FMM.        DIMENSIONAL ANALYSIS
UNIT-III FMM. DIMENSIONAL ANALYSISrknatarajan
 

Último (20)

Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar â‰ŒđŸ” Delhi door step de...
Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar  â‰ŒđŸ” Delhi door step de...Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar  â‰ŒđŸ” Delhi door step de...
Call Now ≜ 9953056974 â‰ŒđŸ” Call Girls In New Ashok Nagar â‰ŒđŸ” Delhi door step de...
 
(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7
(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7
(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7
 
Extrusion Processes and Their Limitations
Extrusion Processes and Their LimitationsExtrusion Processes and Their Limitations
Extrusion Processes and Their Limitations
 
Water Industry Process Automation & Control Monthly - April 2024
Water Industry Process Automation & Control Monthly - April 2024Water Industry Process Automation & Control Monthly - April 2024
Water Industry Process Automation & Control Monthly - April 2024
 
data_management_and _data_science_cheat_sheet.pdf
data_management_and _data_science_cheat_sheet.pdfdata_management_and _data_science_cheat_sheet.pdf
data_management_and _data_science_cheat_sheet.pdf
 
Online banking management system project.pdf
Online banking management system project.pdfOnline banking management system project.pdf
Online banking management system project.pdf
 
UNIT - IV - Air Compressors and its Performance
UNIT - IV - Air Compressors and its PerformanceUNIT - IV - Air Compressors and its Performance
UNIT - IV - Air Compressors and its Performance
 
(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7
(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7
(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7
 
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
 
UNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICS
UNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICSUNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICS
UNIT-IFLUID PROPERTIES & FLOW CHARACTERISTICS
 
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELLPVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
 
Booking open Available Pune Call Girls Koregaon Park 6297143586 Call Hot Ind...
Booking open Available Pune Call Girls Koregaon Park  6297143586 Call Hot Ind...Booking open Available Pune Call Girls Koregaon Park  6297143586 Call Hot Ind...
Booking open Available Pune Call Girls Koregaon Park 6297143586 Call Hot Ind...
 
Coefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptxCoefficient of Thermal Expansion and their Importance.pptx
Coefficient of Thermal Expansion and their Importance.pptx
 
Generative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPTGenerative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPT
 
University management System project report..pdf
University management System project report..pdfUniversity management System project report..pdf
University management System project report..pdf
 
BSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptx
BSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptxBSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptx
BSides Seattle 2024 - Stopping Ethan Hunt From Taking Your Data.pptx
 
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
 
Roadmap to Membership of RICS - Pathways and Routes
Roadmap to Membership of RICS - Pathways and RoutesRoadmap to Membership of RICS - Pathways and Routes
Roadmap to Membership of RICS - Pathways and Routes
 
Intze Overhead Water Tank Design by Working Stress - IS Method.pdf
Intze Overhead Water Tank  Design by Working Stress - IS Method.pdfIntze Overhead Water Tank  Design by Working Stress - IS Method.pdf
Intze Overhead Water Tank Design by Working Stress - IS Method.pdf
 
UNIT-III FMM. DIMENSIONAL ANALYSIS
UNIT-III FMM.        DIMENSIONAL ANALYSISUNIT-III FMM.        DIMENSIONAL ANALYSIS
UNIT-III FMM. DIMENSIONAL ANALYSIS
 

Economic_Load_Dispatch.pdf

  • 1. Economic Load Dispatch I The idea is to minimize the cost of electricity generation without sacrificing quality and reliability. I Therefore, the production cost is minimized by operating plants economically. I Since the load demand varies, the power generation must vary accordingly to maintain the power balance. I The turbine-governor must be controlled such that the demand is met economically. I This arises when there are multiple choices.
  • 2. Economic Distribution of Loads between the units in a Plant: I To determine the economic distribution of load between various generating units, the variable operating costs of the units must be expressed in terms of the power output. I Fuel cost is the principle factor in thermal and nuclear power plants. It must be expressed in terms of the power output. I Operation and Maintenance costs can also be expressed in terms of the power output. I Fixed costs, such as the capital cost, depreciation etc., are not included in the fuel cost.
  • 3. Let us define the input cost of an unit i ,Fi in Rs./h and the power output of the unit as Pi . Then the input cost can be expressed in terms of the power output as Fi = ai P2 i + bi Pi + ci Rs/h Where ai , bi and ci are fuel cost coefficients. The incremental operating cost of each unit is λi = dFi dPi = 2ai Pi + bi Rs./MWh Let us assume that there ar N units in a plant. 1 N PD
  • 4. The total fuel cost is FT = F1 + F2 + · · · + FN = N X i=1 Fi Rs./h All the units have to supply a load demand of PD MW. P1 + P2 + · · · + PN = PD N X i=1 Pi = PD min FT = N X i=1 Fi Subject to N X i=1 Pi = PD
  • 5. It is a constrained optimization problem. Let us form the Lagrangian function. L = FT + λ(PD − N X i=1 Pi ) To find the optimum, ∂L ∂Pi = 0 i = 1, 2, · · · , N ∂L ∂λ = 0 dFi dPi = λ i = 1, 2, · · · , N N X i=1 Pi = PD
  • 6. N + 1 linear equations need to be solved for N + 1 variables. For economical division of load between units within a plant, the criterion is that all units must operate at the same incremental fuel cost. dF1 dP1 = dF2 dP2 = · · · = dFn dPn = λ This is called the coordination equation. P1 (MW) dF 1 dP 1 (Rs/MWhr) P2 (MW) dF 2 dP 2 (Rs/MWhr) λ∗ P∗ 2 P∗ 1
  • 7. Example : Consider two units of a plant that have fuel costs of F1 = 0.2P2 1 + 40P1 + 120 Rs./h F2 = 0.25P2 2 + 30P2 + 150 Rs./h 1. Determine the economic operating schedule and the corresponding cost of generation for the demand of 180 MW. 2. If the load is equally shared by both the units, determine the savings obtained by loading the units optimally.
  • 8. 1. For economical dispatch, dF1 dP1 = dF2 dP2 0.4P1 + 40 = 0.5P2 + 30 and P1 + P2 = 180 On solving the above two equations, P1 = 88.89 MW; P2 = 91.11 MW The cost of generation is FT = F1 + F2 = 10, 214.43 Rs./h
  • 9. 2. If the load is shared equally, P1 = 90 MW; P2 = 90 MW The cost of generation is FT = 10, 215 Rs./h Therefore, the saving will be 0.57 Rs./h
  • 10. Generator Limits: The power generation limit of each unit is given by the inequality constraints Pi,min ≀ Pi ≀ Pi,max i = 1, · · · , N I The maximum limit Pmax is the upper limit of power generation capacity of each unit. I Whereas, the lower limit Pmin pertains to the thermal consideration of operating a boiler in a thermal or nuclear generating station. How to consider the limits I If any one of the optimal values violates its limits, fix the generation of that unit to the violated value. I Optimally dispatch the reduced load among the remaining generators.
  • 11. Example: The fuel cost functions for three thermal plants are F1 = 0.4P2 1 + 10P1 + 25 Rs./h F2 = 0.35P2 2 + 5P2 + 20 Rs./h F3 = 0.475P2 3 + 15P3 + 35 Rs./h The generation limits of the units are 30 MW ≀ P1 ≀ 500 MW 30 MW ≀ P2 ≀ 500 MW 30 MW ≀ P3 ≀ 250 MW Find the optimum schedule for the load of 1000 MW.
  • 12. For optimum dispatch, dF1 dP1 = dF2 dP2 = dF3 dP3 0.8P1 + 10 = 0.7P2 + 5 0.7P2 + 5 = 0.9P3 + 15 and P1 + P2 + P3 = 1000 On solving the above three equations, P1 = 334.3829 MW; P2 = 389.2947 MW; P3 = 276.3224 MW Since the unit 3 violates its maximum limit, P3 = 250 MW
  • 13. The remaining load (750 MW) is scheduled optimally among 1 and 2 units. 0.8P1 + 10 = 0.7P2 + 5 P1 + P2 = 750 On solving the above equations, P1 = 346.6667 MW; P2 = 403.3333 MW Therefore, the final load distribution is P1 = 346.6667 MW; P2 = 403.3333 MW; P3 = 250 MW
  • 14. Economic Distribution of Loads between different Plants: I If the plants are spread out geographically, line losses must be considered. I The line losses are expressed as a function of generator outputs. min FT = N X i=1 Fi Subject to N X i=1 Pi = PL + PD where PL = f (Pi ). It is a nonlinear function of Pi . Let us form the Lagrangian function. L = FT + λ(PD + PL − N X i=1 Pi )
  • 15. To find the optimum, ∂L ∂Pi = 0 i = 1, 2, · · · , N ∂L ∂λ = 0 dFi dPi + λ ∂PL ∂Pi = λ i = 1, 2, · · · , N dFi dPi = λ 1 − ∂PL ∂Pi 1 1 − ∂PL ∂Pi dFi dPi = λ Let us define the penalty factor Li for ith generator. Li dFi dPi = λ
  • 16. where Li = 1 1 − ∂PL ∂Pi . For economical division of load between plants, the criterion is L1 dF1 dP1 = L2 dF2 dP2 = · · · = Ln dFn dPn = λ This is called the exact coordination equation. Since PL is a nonlinear function of Pi , the following N + 1 equations need to be solved numerically for N + 1 variables. Li dFi dPi = λ i = 1, 2, · · · , N N X i=1 Pi = PL + PD
  • 17. The transmission losses are usually expressed as PL = PT BP where P = [P1, P2, · · · Pn] and B is a symmetric matrix given by B = ïŁź ïŁŻ ïŁŻ ïŁŻ ïŁ° B11 B12 · · · B1n B21 B22 · · · B2n . . . . . . ... . . . Bn1 Bn2 · · · Bnn ïŁč ïŁș ïŁș ïŁș ïŁ» The elements of the matrix B are called the loss coefficients.
  • 18. Example: Consider a two bus system. 1 O 2 O Load P1 P2 The incremental fuel cost characteristics of plant 1 and plant 2 are given by dF1 dP1 = 0.025P1 + 14 Rs/MWHr dF2 dP2 = 0.05P2 + 16 Rs/MWHr If 200 MW of power is transmitted from plant 1 to the load, a transmission loss of 20 MW will be incurred. Find the optimum generation schedule and the cost of received power for a load demand of 204.41 MW.
  • 19. PL = P1 P2 B11 B12 B21 B22 P1 P2 Since the load is at bus 2, P2 will not have any effect on PL. B12 = B21 = 0; B22 = 0 Therefore, PL = B11P2 1 For 200 MW of P1, PL = 20 MW. 20 = B112002 B11 = 0.0005 MW−1 PL = 0.0005P2 1
  • 20. For optimum dispatch, L1 dF1 dP1 = L2 dF2 dP2 = λ Since PL is a function of P1 alone, L1 = 1 1 − ∂PL ∂P1 = 1 1 − 0.001P1 L2 = 1 1 1 − 0.001P1 0.025P1 + 14 = 0.05P2 + 16 On simplification, 0.041P1 − 0.05P2 + 0.00005P1P2 = 2 and P1 + P2 − 0.0005P2 1 = 204.41
  • 21. f1(P1, P2) = 2 f2(P1, P2) = 204.41 Let us solve them by N-R method. ∆f = J∆P where ∆f = 2 − f1(P1, P2) 204.41 − f2(P1, P2) J = ïŁź ïŁŻ ïŁ° ∂f1 ∂P1 ∂f1 ∂P2 ∂f2 ∂P1 ∂f2 ∂P2 ïŁč ïŁș ïŁ»
  • 22. To find the initial estimate : Let us solve the problem with out loss. 0.025P1 + 14 = 0.05P2 + 16 P1 + P2 = 204.41 P0 1 = 162.94; P0 2 = 41.47 First Iteration : ∆f0 = 2 − f1(P0 1 , P0 2 ) 204.41 − f2(P0 1 , P0 2 ) = −2.9449 13.2747 J0 = 0.0431 −0.0419 0.8371 0.9585 ∆P0 1 ∆P0 2 = −29.7060 39.7906 P1 1 P1 2 = P0 1 P0 2 + ∆P0 1 ∆P0 2 = 133.2340 81.2606
  • 23. It took 6 iterations to converge. P1 = 133.3153 MW P2 = 79.9812 MW The cost of received power is λ = L2 dF2 dP2 = 1 × (0.05 × 79.9812 + 16) = 19.9991 Rs./MWh
  • 24. λ-iteration Method PL = N X i=1 N X j=1 Pi Bij Pj The exact coordination equation is dFi dPi + λ ∂PL ∂Pi = λ It can be written as 2ai Pi + bi + 2λ N X j=1 Bij Pj = λ 2ai Pi + bi + 2λBii Pi + 2λ N X j=1 j6=i Bij Pj = λ
  • 25. Pi = λ − bi − 2λ PN j=1 j6=i Bij Pj 2(ai + λBii ) On substituting this in the power balance equation, N X i=1 Pi = PD + PL N X i=1 λ − bi − 2λ PN j=1 j6=i Bij Pj 2(ai + λBii ) = PD + PL f (λ) = PD + PL This needs to be solved repeatedly for different values of λ.
  • 26. Expanding it using Taylor’s series about an initial point (λ0) and neglecting the higher order terms. f (λ0 ) + ( df (λ) dλ )0 ∆λ0 ≈ PD + P0 L ∆λ0 = PD + P0 L − f (λ0) (df (λ) dλ )0 where f (λ0 ) = N X i=1 P0 i ( df (λ) dλ )0 = N X i=1 ( dPi dλ )0 = N X i=1 ïŁ« ïŁŹ ïŁ­ ai + bi Bii − 2ai PN j=1 j6=i Bij P0 j 2(ai + λ0Bii )2 ïŁ¶ ïŁ· ïŁž Therefore, λ1 = λ0 + ∆λ0
  • 27. In general, λk+1 = λk + ∆λk where ∆λk = PD + Pk L − PN i=1 Pk i PN i=1 ïŁ« ïŁ­ ai +bi Bii −2ai PN j=1 j6=i Bij Pk j 2(ai +λk Bii )2 ïŁ¶ ïŁž I Start with λk. I Find Pk i as follows: Pk i = λk − bi − 2λk PN j=1 j6=i Bij Pk j 2(ai + λkBii )
  • 28. I Find Pk L using the following equation. Pk L = N X i=1 N X j=1 Pk i Bij Pk j I Repeat the above steps till |PD + Pk L − PN i=1 Pk i | ≀ . I To start with, assume λ0 such that it is greater than the largest value of the coefficients b.
  • 29. Example : Let us take the same example. The incremental fuel cost characteristics of plant 1 and plant 2 are given by dF1 dP1 = 0.025P1 + 14 Rs/MWHr dF2 dP2 = 0.05P2 + 16 Rs/MWHr PL = 0.0005P2 1 1. Assume λ0 = 17. 2. P0 1 and P0 2 are P0 1 = λ0 − b1 2(a1 + λ0B11) = 71.4286 MW P0 2 = λ0 − b2 2(a2) = 20 MW 3. It took 8 iterations to converge. λ = 19.9991 Rs/MWhr P1 = 133.3152 MW P2 = 79.9812 MW