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 1 INTRODUCTION / LITERATURE REVIE
 2 DEFINIATION
 3 PROCEDURE / WORKING
 4 PRINCIPLE
 5 SPECIAL FEATURE
 6 INDUSTRIAL APPLICATION
 7 ADVANTAGE
 8 DISADVANTAGE
 9 RECENT TREADS / FUTURE SCOPE
 10 CONCLUSION
 11 REFERENCE
 Development of cascade converters with new control
strategies is coming up to increase the power pro-
cessing capability and to improve the reliability of
the power electronic system. Particularly, aeronau-
tics and telecommunication appliances require large
conversion ratios. These requirements can be
fulfilled either with the help of isolated step-down/
step-up pulse width modulated (PWM) dc-dc
converters or non-isolated converters. However, the
use of step- down/ step-up converters with
transformers, isolated converters, results in large
switching surges that may damage the switching
devices [l-21. Further, use of transformer limits the
switching frequency of the con- verter. An alternative
option, for realizing larger dc conversion ratios, is
cascading of the converters
 - In this paper signal flow graph non- linear
modeling of cascade boost converters is pre-
sented. TJnified signal flow graph model of the
con- verter is developed and then deduction of
large, small- signal and steady-state models from
the unified graph is demonstrated. Converter
performance expressions are derived. Large-signal
model is developed and programmed in TUTSIM
simulator. Large-signal re- sponses against supply
and load disturbances are ob- tained. Validity of
the proposed SFG modeling is verified through
PSIM simulator result
 Objectives of this chapter zTo learn how to represent
multiple subsystems via block diagramsor signal-flow
graphs. zTo be able to reduce either the block diagram
representation or the signal-flow graph representation to
a single transfer function. „Mason’s rule was used to
derive the system’s transfer function from the signal-flow
graph. This formula replaced block diagram reduction
techniques. „Systems in state space can be represented
using different sets of variables. zPhase-variable,
cascade, parallel, controller canonical, and observer
canonical forms. zA particular representation may be
chosen because one set of state variables has a different
physical meaning than another set, or because of the
ease with which particular state equations can be solved
 How to reduce a block diagram „How to analyze
and design for transient response „How to
represent in state space a system consisting of
multiple subsystems „How to convert between
alternate representations of a system in state
space
i) Switching elements of the basic converter cells are
assumed to be ideal.
 (ii) The individual cells of the cascade converter system
operate in the continuous inductor current mode.
 (iii) The switches SI, S2 operate in synchronism fashion.
 (iv) The ESR of the capacitance and stray ca- pacitances
are neglected
 1. Move from left to right across the lozenge diagram
starting with a value or modied value from the y-column.
 2. One moves in a straight line path to the next column
of the lozenge dia- gram. This straight line path can be
either diagonally upward, horizontal or diagonally
downward.
 In this paper, the SFG approach was extended to
model the dc-dc cascade boost converters operating
in continuous current mode. Large, small- signal and
steady-state models lead to simple graphical circuits
that are very much suitable for analysis and simula-
tion. To confirm the modelling method theoretical
results, obtained from SFG analysis, were compared
with PSIM simulations. They are in close agreement
with each other.
 [1] R. D. Middlebrook, "Transformerless dc-tedc
converters with large conversion ratios," Proc. of
IEEE INTELEC Conference, pp. 455-460, 1984.
 [2] J. A. Morales - Saldana, E. E. Carbajal Gutierrez,
J. Leyva - Ranos, "Modelling of Switch-mode dc-dc
cascade con- verters," IEEE Trans. On Aerospace
and Electronic Sys- tems, Vol. 38(1), pp. 295-299,
2002.
 [3] R. D. Middlebrook, Slobodan Cuk, "A General
Uni- fied Approach to Modeling Switching Converter
Power Stages," IEEE Power Electronics Specialist
Conference, V01.4, pp. 18-34, 1976.
12

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(K 10619) krishna murari yadav (mel-312)[mech. measurment control theory & application

  • 1.
  • 2.  1 INTRODUCTION / LITERATURE REVIE  2 DEFINIATION  3 PROCEDURE / WORKING  4 PRINCIPLE  5 SPECIAL FEATURE  6 INDUSTRIAL APPLICATION  7 ADVANTAGE  8 DISADVANTAGE  9 RECENT TREADS / FUTURE SCOPE  10 CONCLUSION  11 REFERENCE
  • 3.  Development of cascade converters with new control strategies is coming up to increase the power pro- cessing capability and to improve the reliability of the power electronic system. Particularly, aeronau- tics and telecommunication appliances require large conversion ratios. These requirements can be fulfilled either with the help of isolated step-down/ step-up pulse width modulated (PWM) dc-dc converters or non-isolated converters. However, the use of step- down/ step-up converters with transformers, isolated converters, results in large switching surges that may damage the switching devices [l-21. Further, use of transformer limits the switching frequency of the con- verter. An alternative option, for realizing larger dc conversion ratios, is cascading of the converters
  • 4.  - In this paper signal flow graph non- linear modeling of cascade boost converters is pre- sented. TJnified signal flow graph model of the con- verter is developed and then deduction of large, small- signal and steady-state models from the unified graph is demonstrated. Converter performance expressions are derived. Large-signal model is developed and programmed in TUTSIM simulator. Large-signal re- sponses against supply and load disturbances are ob- tained. Validity of the proposed SFG modeling is verified through PSIM simulator result
  • 5.  Objectives of this chapter zTo learn how to represent multiple subsystems via block diagramsor signal-flow graphs. zTo be able to reduce either the block diagram representation or the signal-flow graph representation to a single transfer function. „Mason’s rule was used to derive the system’s transfer function from the signal-flow graph. This formula replaced block diagram reduction techniques. „Systems in state space can be represented using different sets of variables. zPhase-variable, cascade, parallel, controller canonical, and observer canonical forms. zA particular representation may be chosen because one set of state variables has a different physical meaning than another set, or because of the ease with which particular state equations can be solved
  • 6.  How to reduce a block diagram „How to analyze and design for transient response „How to represent in state space a system consisting of multiple subsystems „How to convert between alternate representations of a system in state space
  • 7.
  • 8. i) Switching elements of the basic converter cells are assumed to be ideal.  (ii) The individual cells of the cascade converter system operate in the continuous inductor current mode.  (iii) The switches SI, S2 operate in synchronism fashion.  (iv) The ESR of the capacitance and stray ca- pacitances are neglected
  • 9.  1. Move from left to right across the lozenge diagram starting with a value or modied value from the y-column.  2. One moves in a straight line path to the next column of the lozenge dia- gram. This straight line path can be either diagonally upward, horizontal or diagonally downward.
  • 10.  In this paper, the SFG approach was extended to model the dc-dc cascade boost converters operating in continuous current mode. Large, small- signal and steady-state models lead to simple graphical circuits that are very much suitable for analysis and simula- tion. To confirm the modelling method theoretical results, obtained from SFG analysis, were compared with PSIM simulations. They are in close agreement with each other.
  • 11.  [1] R. D. Middlebrook, "Transformerless dc-tedc converters with large conversion ratios," Proc. of IEEE INTELEC Conference, pp. 455-460, 1984.  [2] J. A. Morales - Saldana, E. E. Carbajal Gutierrez, J. Leyva - Ranos, "Modelling of Switch-mode dc-dc cascade con- verters," IEEE Trans. On Aerospace and Electronic Sys- tems, Vol. 38(1), pp. 295-299, 2002.  [3] R. D. Middlebrook, Slobodan Cuk, "A General Uni- fied Approach to Modeling Switching Converter Power Stages," IEEE Power Electronics Specialist Conference, V01.4, pp. 18-34, 1976.
  • 12. 12