EE6604
DESIGNOF ELECTRICAL MACHINES
ELECTRICAL AND ELECTRONICS ENGINEERING
SRI KRISHNA KUMAR S
HTS953
AP/EEE
UNITII DC MACHINES
Output Equations
1 1
11
Main Dimensions
Choice of Specific Electric and Magnetic Loading 1 1
Magnetic Circuits Calculations
1 1Carter’s Coefficient
Net length of Iron
Real & Apparent flux densities
1
1
Selection of number of poles 1
Design of Armature
1
Design of commutator and brushes
Performance prediction using design values 1
2.1. Output equation of a DC machine
Output equation relates the output and main dimensions of the machine. Actually it relates the power developed in the
armature and main dimensions.
E : EMF induced or back EMF
Ia : armature current
Φ:Average value of flux / pole
Z : Total number of armature conductors
N : Speed in rpm
n : Speed in rps
P : Number of poles
A : number of armature paths or circuits
D : Diameter of the armature
L : Length of the armature core
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
2.1. Output equation of a DC machine
2.1. Output equation of a DC machine
•Find the dimensions of a 200kW, 250V, 6 pole, 1000 rpm DC generator. The maximum value
of flux density in air gap is 0.87wb/m2 and the ampere conductors per metre length of
armature periphery are 31000. Ratio of pole arc to pole pitch is 0.67 and efficiency 91%.
Assume that the ratio of core length to pole pitch = 0.75. (AU MAY 2008)
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
=(Pφ)×(IaZ/A)×N x 10-3/60
=(Pφ)×(IaZ/A)×n x 10-3....... (1)
The term P φ represents the total flux and is called the magnetic loading. Magnetic
Loading per unit area of the armature surface is called the specific magnetic loading or average value of the
flux density in the air gap Bav.
2.1. Output equation of a DC machine
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
=(Pφ)×(IaZ/A)×N x 10-3/60
=(Pφ)×(IaZ/A)×n x 10-3....... (1)
The term P φ represents the total flux and is called the magnetic loading. Magnetic
Loading per unit area of the armature surface is called the specific magnetic loading or average value of the
flux density in the air gap Bav.
Bav = Pφ /π DL Wb/m2 or tesla denoted by T
Therefore Pφ = Bav π DL ................ (2)
2.1. Output equation of a DC machine
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
=(Pφ)×(IaZ/A)×N x 10-3/60
=(Pφ)×(IaZ/A)×n x 10-3....... (1)
The term P φ represents the total flux and is called the magnetic loading. Magnetic
Loading per unit area of the armature surface is called the specific magnetic loading or average value of the
flux density in the air gap Bav. That is,
Bav = Pφ /π DL Wb/m2 or tesla denoted by T
Therefore Pφ = Bav π DL ................ (2)
The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading.
2.1. Output equation of a DC machine
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
=(Pφ)×(IaZ/A)×N x 10-3/60
=(Pφ)×(IaZ/A)×n x 10-3....... (1)
The term P φ represents the total flux and is called the magnetic loading. Magnetic
Loading per unit area of the armature surface is called the specific magnetic loading or average value of the
flux density in the air gap Bav. That is,
Bav = Pφ /π DL Wb/m2 or tesla denoted by T
Therefore Pφ = Bav π DL ................ (2)
The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading.
Electric loading/unit length of armature periphery is called the specific electric loading q. That is,
q= IaZ / π A D Amp-cond / m
2.1. Output equation of a DC machine
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
=(Pφ)×(IaZ/A)×N x 10-3/60
=(Pφ)×(IaZ/A)×n x 10-3....... (1)
The term P φ represents the total flux and is called the magnetic loading. Magnetic
Loading per unit area of the armature surface is called the specific magnetic loading or average value of the
flux density in the air gap Bav. That is,
Bav = Pφ /π DL Wb/m2 or tesla denoted by T
Therefore Pφ = Bav π DL ................ (2)
The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading.
Electric loading/unit length of armature periphery is called the specific electric loading q. That is,
q= IaZ / π A D Amp-cond / m
Therefore Ia Z/A = q π D ............ (3)
2.1. Output equation of a DC machine
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
=(Pφ)×(IaZ/A)×N x 10-3/60
=(Pφ)×(IaZ/A)×n x 10-3....... (1)
The term P φ represents the total flux and is called the magnetic loading. Magnetic
Loading per unit area of the armature surface is called the specific magnetic loading or average value of the
flux density in the air gap Bav. That is,
Bav = Pφ /π DL Wb/m2 or tesla denoted by T
Therefore Pφ = Bav π DL ................ (2)
The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading.
Electric loading/unit length of armature periphery is called the specific electric loading q. That is,
q= IaZ / π A D Amp-cond / m
Therefore Ia Z/A = q π D ............ (3)
Substitution of equations 2 and 3 in 1, leads to
kW = Bav π DL × q π D × (n × 10-3)
2.1. Output equation of a DC machine
Power developed in the armature in kW, Pa= E Ia x 10-3
=(φZNP/60 A)× Ia× 10-3
=(Pφ)×(IaZ/A)×N x 10-3/60
=(Pφ)×(IaZ/A)×n x 10-3....... (1)
The term P φ represents the total flux and is called the magnetic loading. Magnetic
Loading per unit area of the armature surface is called the specific magnetic loading or average value of the
flux density in the air gap Bav. That is,
Bav = Pφ /π DL Wb/m2 or tesla denoted by T
Therefore Pφ = Bav π DL ................ (2)
The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading.
Electric loading/unit length of armature periphery is called the specific electric loading q. That is,
q= IaZ / π A D Amp-cond / m
Therefore Ia Z/A = q π D ............ (3)
Substitution of equations 2 and 3 in 1, leads to
kW = Bav π DL × q π D × (n × 10-3)
= B q D2 L n
= π2Bav q C0 D2 L N 10-3
Where C0= π2Bav q 10-3 is called the output coefficeint of the DC machine
2.1. Output equation of a DC machine

More Related Content

PPSX
3.1. OUTPUT EQUATION
PPTX
Transformer design (220-110)V 100 VA
PDF
Transformer
PPT
ECNG 3013 B
PPT
ECNG 3013 C
PPT
Transmission line By Lipun
DOCX
Low pass filter and Integrator
PDF
Powerelectronics questionbank
3.1. OUTPUT EQUATION
Transformer design (220-110)V 100 VA
Transformer
ECNG 3013 B
ECNG 3013 C
Transmission line By Lipun
Low pass filter and Integrator
Powerelectronics questionbank

What's hot (19)

PPT
ECNG 3013 D
PPTX
Calculations of a.c distributions methods & 3 phase unbalanced loads &amp...
PPT
Rc and rl differentiator and integrator circuit
PDF
امتحان جهد عالي 2016
PPTX
Electrical Circuits
PPTX
Inverter
PDF
Design of two stage OPAMP
DOCX
Transmission and distribution line design final
PPT
Power Electronics Chapter 7
PPT
Dtdm theory book soft copy 2
PPTX
Electrostatics
PPT
Rlc circuits det2033 chp2
PPT
Project review
PPT
Lecture 2
PDF
A novel voltage reference without the operational amplifier and resistors
PDF
Chapter 12 1 microelectronics
PDF
The RC Circuit
PPT
Series parallel ac rlc networks
PDF
Balaji mini proj
ECNG 3013 D
Calculations of a.c distributions methods & 3 phase unbalanced loads &amp...
Rc and rl differentiator and integrator circuit
امتحان جهد عالي 2016
Electrical Circuits
Inverter
Design of two stage OPAMP
Transmission and distribution line design final
Power Electronics Chapter 7
Dtdm theory book soft copy 2
Electrostatics
Rlc circuits det2033 chp2
Project review
Lecture 2
A novel voltage reference without the operational amplifier and resistors
Chapter 12 1 microelectronics
The RC Circuit
Series parallel ac rlc networks
Balaji mini proj
Ad

Similar to EE6604 unit2 (20)

PDF
Review_of_EMF_and_Torque_Equations.pdf xx
PDF
Dc electrcial machine generator and its type
PPT
Dcmachine 1233234542827948-3
PPT
Dcmachine 1233234542827948-3-1
PPT
Dcmachine 1233234542827948-3-2
PDF
DC MachinesDC MachinesDC MachinesDC MachinesDC MachinesDC MachinesDC Machines...
PDF
EE6604 Dem Rejinpaul_iQ_May.June_2016
PPTX
D C MOTOR LECTURE electrical engineering.pptx
PPTX
Unit-II PPT basics for engineering students
PPTX
DC Machinesmechnacial engernerring .pptx
PPTX
BEEM UII.pptx
PPTX
BATCH 5 final.pptxvdihfirehgvrhgvkrhgkrjhgkrjehguh
PPTX
Dc machines ppt
PPTX
9884Lecture 3.pptx on dc generator it's
PDF
BEEE machines
PPTX
Basic Electrical and Electronics Engineering.pptx
PPTX
Basic Electrical and Electronics Engineering.pptx
PDF
performance of dc machine especially dc gen
PPT
Dcmachine
Review_of_EMF_and_Torque_Equations.pdf xx
Dc electrcial machine generator and its type
Dcmachine 1233234542827948-3
Dcmachine 1233234542827948-3-1
Dcmachine 1233234542827948-3-2
DC MachinesDC MachinesDC MachinesDC MachinesDC MachinesDC MachinesDC Machines...
EE6604 Dem Rejinpaul_iQ_May.June_2016
D C MOTOR LECTURE electrical engineering.pptx
Unit-II PPT basics for engineering students
DC Machinesmechnacial engernerring .pptx
BEEM UII.pptx
BATCH 5 final.pptxvdihfirehgvrhgvkrhgkrjhgkrjehguh
Dc machines ppt
9884Lecture 3.pptx on dc generator it's
BEEE machines
Basic Electrical and Electronics Engineering.pptx
Basic Electrical and Electronics Engineering.pptx
performance of dc machine especially dc gen
Dcmachine
Ad

Recently uploaded (20)

PPTX
6ME3A-Unit-II-Sensors and Actuators_Handouts.pptx
PDF
737-MAX_SRG.pdf student reference guides
PPTX
Fundamentals of safety and accident prevention -final (1).pptx
PPTX
Chemical Technological Processes, Feasibility Study and Chemical Process Indu...
PPTX
CURRICULAM DESIGN engineering FOR CSE 2025.pptx
PDF
Improvement effect of pyrolyzed agro-food biochar on the properties of.pdf
PPTX
Graph Data Structures with Types, Traversals, Connectivity, and Real-Life App...
PDF
Categorization of Factors Affecting Classification Algorithms Selection
PDF
Soil Improvement Techniques Note - Rabbi
PDF
22EC502-MICROCONTROLLER AND INTERFACING-8051 MICROCONTROLLER.pdf
PPTX
Software Engineering and software moduleing
PDF
BIO-INSPIRED ARCHITECTURE FOR PARSIMONIOUS CONVERSATIONAL INTELLIGENCE : THE ...
PDF
Influence of Green Infrastructure on Residents’ Endorsement of the New Ecolog...
PPTX
Fundamentals of Mechanical Engineering.pptx
PPTX
CyberSecurity Mobile and Wireless Devices
PDF
Visual Aids for Exploratory Data Analysis.pdf
PDF
Level 2 – IBM Data and AI Fundamentals (1)_v1.1.PDF
PPTX
tack Data Structure with Array and Linked List Implementation, Push and Pop O...
PDF
Exploratory_Data_Analysis_Fundamentals.pdf
PDF
ChapteR012372321DFGDSFGDFGDFSGDFGDFGDFGSDFGDFGFD
6ME3A-Unit-II-Sensors and Actuators_Handouts.pptx
737-MAX_SRG.pdf student reference guides
Fundamentals of safety and accident prevention -final (1).pptx
Chemical Technological Processes, Feasibility Study and Chemical Process Indu...
CURRICULAM DESIGN engineering FOR CSE 2025.pptx
Improvement effect of pyrolyzed agro-food biochar on the properties of.pdf
Graph Data Structures with Types, Traversals, Connectivity, and Real-Life App...
Categorization of Factors Affecting Classification Algorithms Selection
Soil Improvement Techniques Note - Rabbi
22EC502-MICROCONTROLLER AND INTERFACING-8051 MICROCONTROLLER.pdf
Software Engineering and software moduleing
BIO-INSPIRED ARCHITECTURE FOR PARSIMONIOUS CONVERSATIONAL INTELLIGENCE : THE ...
Influence of Green Infrastructure on Residents’ Endorsement of the New Ecolog...
Fundamentals of Mechanical Engineering.pptx
CyberSecurity Mobile and Wireless Devices
Visual Aids for Exploratory Data Analysis.pdf
Level 2 – IBM Data and AI Fundamentals (1)_v1.1.PDF
tack Data Structure with Array and Linked List Implementation, Push and Pop O...
Exploratory_Data_Analysis_Fundamentals.pdf
ChapteR012372321DFGDSFGDFGDFSGDFGDFGDFGSDFGDFGFD

EE6604 unit2

  • 1. EE6604 DESIGNOF ELECTRICAL MACHINES ELECTRICAL AND ELECTRONICS ENGINEERING SRI KRISHNA KUMAR S HTS953 AP/EEE
  • 2. UNITII DC MACHINES Output Equations 1 1 11 Main Dimensions Choice of Specific Electric and Magnetic Loading 1 1 Magnetic Circuits Calculations 1 1Carter’s Coefficient Net length of Iron Real & Apparent flux densities 1 1 Selection of number of poles 1 Design of Armature 1 Design of commutator and brushes Performance prediction using design values 1
  • 3. 2.1. Output equation of a DC machine Output equation relates the output and main dimensions of the machine. Actually it relates the power developed in the armature and main dimensions. E : EMF induced or back EMF Ia : armature current Φ:Average value of flux / pole Z : Total number of armature conductors N : Speed in rpm n : Speed in rps P : Number of poles A : number of armature paths or circuits D : Diameter of the armature L : Length of the armature core
  • 4. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 2.1. Output equation of a DC machine
  • 5. 2.1. Output equation of a DC machine •Find the dimensions of a 200kW, 250V, 6 pole, 1000 rpm DC generator. The maximum value of flux density in air gap is 0.87wb/m2 and the ampere conductors per metre length of armature periphery are 31000. Ratio of pole arc to pole pitch is 0.67 and efficiency 91%. Assume that the ratio of core length to pole pitch = 0.75. (AU MAY 2008)
  • 6. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 =(Pφ)×(IaZ/A)×N x 10-3/60 =(Pφ)×(IaZ/A)×n x 10-3....... (1) The term P φ represents the total flux and is called the magnetic loading. Magnetic Loading per unit area of the armature surface is called the specific magnetic loading or average value of the flux density in the air gap Bav. 2.1. Output equation of a DC machine
  • 7. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 =(Pφ)×(IaZ/A)×N x 10-3/60 =(Pφ)×(IaZ/A)×n x 10-3....... (1) The term P φ represents the total flux and is called the magnetic loading. Magnetic Loading per unit area of the armature surface is called the specific magnetic loading or average value of the flux density in the air gap Bav. Bav = Pφ /π DL Wb/m2 or tesla denoted by T Therefore Pφ = Bav π DL ................ (2) 2.1. Output equation of a DC machine
  • 8. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 =(Pφ)×(IaZ/A)×N x 10-3/60 =(Pφ)×(IaZ/A)×n x 10-3....... (1) The term P φ represents the total flux and is called the magnetic loading. Magnetic Loading per unit area of the armature surface is called the specific magnetic loading or average value of the flux density in the air gap Bav. That is, Bav = Pφ /π DL Wb/m2 or tesla denoted by T Therefore Pφ = Bav π DL ................ (2) The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading. 2.1. Output equation of a DC machine
  • 9. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 =(Pφ)×(IaZ/A)×N x 10-3/60 =(Pφ)×(IaZ/A)×n x 10-3....... (1) The term P φ represents the total flux and is called the magnetic loading. Magnetic Loading per unit area of the armature surface is called the specific magnetic loading or average value of the flux density in the air gap Bav. That is, Bav = Pφ /π DL Wb/m2 or tesla denoted by T Therefore Pφ = Bav π DL ................ (2) The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading. Electric loading/unit length of armature periphery is called the specific electric loading q. That is, q= IaZ / π A D Amp-cond / m 2.1. Output equation of a DC machine
  • 10. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 =(Pφ)×(IaZ/A)×N x 10-3/60 =(Pφ)×(IaZ/A)×n x 10-3....... (1) The term P φ represents the total flux and is called the magnetic loading. Magnetic Loading per unit area of the armature surface is called the specific magnetic loading or average value of the flux density in the air gap Bav. That is, Bav = Pφ /π DL Wb/m2 or tesla denoted by T Therefore Pφ = Bav π DL ................ (2) The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading. Electric loading/unit length of armature periphery is called the specific electric loading q. That is, q= IaZ / π A D Amp-cond / m Therefore Ia Z/A = q π D ............ (3) 2.1. Output equation of a DC machine
  • 11. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 =(Pφ)×(IaZ/A)×N x 10-3/60 =(Pφ)×(IaZ/A)×n x 10-3....... (1) The term P φ represents the total flux and is called the magnetic loading. Magnetic Loading per unit area of the armature surface is called the specific magnetic loading or average value of the flux density in the air gap Bav. That is, Bav = Pφ /π DL Wb/m2 or tesla denoted by T Therefore Pφ = Bav π DL ................ (2) The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading. Electric loading/unit length of armature periphery is called the specific electric loading q. That is, q= IaZ / π A D Amp-cond / m Therefore Ia Z/A = q π D ............ (3) Substitution of equations 2 and 3 in 1, leads to kW = Bav π DL × q π D × (n × 10-3) 2.1. Output equation of a DC machine
  • 12. Power developed in the armature in kW, Pa= E Ia x 10-3 =(φZNP/60 A)× Ia× 10-3 =(Pφ)×(IaZ/A)×N x 10-3/60 =(Pφ)×(IaZ/A)×n x 10-3....... (1) The term P φ represents the total flux and is called the magnetic loading. Magnetic Loading per unit area of the armature surface is called the specific magnetic loading or average value of the flux density in the air gap Bav. That is, Bav = Pφ /π DL Wb/m2 or tesla denoted by T Therefore Pφ = Bav π DL ................ (2) The term (Ia Z/A) represents the total ampere-conductors on the armature and is called the electric loading. Electric loading/unit length of armature periphery is called the specific electric loading q. That is, q= IaZ / π A D Amp-cond / m Therefore Ia Z/A = q π D ............ (3) Substitution of equations 2 and 3 in 1, leads to kW = Bav π DL × q π D × (n × 10-3) = B q D2 L n = π2Bav q C0 D2 L N 10-3 Where C0= π2Bav q 10-3 is called the output coefficeint of the DC machine 2.1. Output equation of a DC machine