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International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
DOI : 10.5121/ijccms.2013.2304 39
OPTIMIZATION OF ARTIFICIAL NEURAL NETWORK
MODEL FOR IMPROVEMENT OF ARTIFICIAL
INTELLIGENCE OF MANUALLY DRIVEN BRICK
MAKING MACHINE POWERED BY HPFM
P. A. Chandak1
and J. P. Modak2
1
Department of Mechanical Engineering, DMIETR, Wardha (MH), India
2
Professor Emeritus, Dean (R&D), PCE, Nagpur(MH), India
ABSTRACT
Considerable development has been done by some authors of this paper towards development of
manufacturing process units energized by Human Powered Flywheel Motor (HPFM) as an energy source.
This machine system comprises three sub systems namely (i) HPFM (ii) Torsionally Flexible Clutch (TFC)
(iii) A Process Unit. Process unit so far tried are mostly rural based such as brick making machine (both
rectangular and keyed cross sectioned), Low head water lifting, Wood turning, Wood strips cutting, etc
HPFM comprises pedalling system similar to bicycle, a speed rising gear pair and a flywheel big enough
such that a young lad of 21-25 years, 165cm height, slim structure can pump energy around 30,000 N-m in
minutes time. Once such an energy is stored peddling is stopped and a special type of TFC is engaged
which very efficiently brings about momentum and energy transfer from flywheel to a process unit. Process
unit utilization time upon clutch engagement is 5 to 15 seconds depending on the application. In other word
process units needing power of order of 3 hp to 10 hp can be powered by such a machine concept.
Experimental data base model is formulated for Human Powered Flywheel Motor Energized Brick Making
Machine (HPFMEBMM).
The focus of the present paper is on development of an optimum Artificial Neural Network (ANN) model
which will predict the experimental evidences accurately and precisely. The optimisation is acknowledged
though variation of various parameters of ANN topology like training algorithm, learning algorithm, size
of hidden layer, number of hidden layers, etc while training the network and accepting the best value of
that parameter. The paper also discusses the effects and results of variation of various parameters on
prediction of network.
KEYWORDS
ANN, Matlab, Manually driven brick making machine. Simulation.
1. REVIEW OF THE BRICK MAKING MACHINE AND ITS PROCESS UNIT
1.1 Working of manually driven Brick making machine
A manually driven Auger-type brick making [1][3] machine developed by Dr. J. P. Modak is as
shown in figure. The operator drives the flywheel (17) though chain (25) and a pair of gears (19,
20). The chain drive is utilized for first stage transmission because the drive is required to be
irreversible. This is achieved with the conventional bicycle drive with a free wheel (21). When
the flywheel attains sufficient speed, the single jaw clutch (13, 15) is engaged. The clutch drives
the auger screw through a pair of gears (9, 10). The mix fed through hopper (3). A cone (2)
connects the drum (30) to the die (1). The cone eliminates the rotary motion of the mix before it
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
40
enters the die. The extracted column is collected in a detachable mould (4). It is lined on the
inside by Perspex to provide least resistance to motion of the column. The column is subsequently
demoulded by placing it upside down on the platform. The mould is moved horizontally, leaving
the column on the platform. About one or two hours after the column is laid on the platform, it
becomes stiff enough to be cut by a cutter to form bricks of standard size.
1.DIE, 2.CONE, 3.HOPPER, 4.AL MOULD, 5.MOULDING STAND, 6.CONVEYOR SCREW, 7.CONVEYER SHAFT,
8.HOPPER, 9. GEAR, 10.PINION, 11.PINION SHAFT, 12.BEARING, MOVABLE HALF CLUTCH, 14.CLUTCH LEVER,
15.FIXED HALF CLUTCH, 16.FLYWHEEL SHAFT, 17.FLYWHEEL, 18, BEARING FOR FLYWHEEL, 19.PINION II, 20.GEAR
II, 21.FREWHELL, 22.INTERMEDIATE SHAFT, 23.BEARING FOR INTERMEDIATE SHAFT, 24.CRANK GEAR, 25.PINION
FOLLOWER CHAIN, 26.DRIVER SEAT, 27.HANDLE, 28.BRACKET, 29.FRAME, 30.CONVEYOR DRUM.
Figure 1. Manually driven Brick Making Machine
The following process variables were involved in the process of experimentation. [1]
Table 1. Process variables and their dimensions
Sr No. Description of variables
Type of
variable
Symbol Dimension
1 Weight of lime Independent WL ML-1T-2
2 Weight of sand Independent Ws ML-1T-2
3 Weight of flyash Independent Wf ML-1T-2
4 Weight of water Independent Ww ML-1T-2
5 Outside diameter of screw Independent D1 L
6 Inside diameter of screw Independent D2 L
7 Pitch of Screw Independent P L
8 Larger Diameter of Cone Independent D1 L
9 Smaller Diameter of Cone Independent D3 L
10 Length of cone Independent LC L
11 Length of die Independent LD L
12 Moment of Inertia of flywheel Independent I ML2
13 Angular velocity of flywheel Independent W T-1
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
41
14 Acceleration of due to gravity Independent G LT-2
15 Gear ratio Independent G -
16 Length of square side of die Independent S L
17 Strength of brick Dependent Sb ML-1T-2
18 Length of Extruded Brick Column Dependent Lb L
19 Time of Extrusion Dependent Te T
20
Maximum length of Extruded Brick
Column
Dependent Lbm L
21 Critical Pressure of Extrusion Dependent Pc ML-1T-2
22 Instantaneous Torque on the angular shaft Dependent T ML-1T-2
1.2. Experimental setup
The experimental setup [1] basically consists of a manually driven brick making machine with
following facilities
 Facility to change die, cone, auger, screw, blades and gears
 Facility to mount the torque meter and to record process torque during extrusion process.
 Facility to mount technogerators to record speeds of flywheel and auger screw.
1.3. Procedure of Experimentation
Initially the machine parameters were set as per the plan of experimentation. A homogeneous mix
of lime-flyash-sand, in requisite proportion by weight, was prepared by adding suitable amount of
water. The mix was soaked for 48 hours and was kept ready for use. To assure thorough mixing,
die and cone machine were removed. Sufficient mix was fed into the hopper.
The flywheel was speeded up to 400 rpm and the clutch was engaged. The mix passes out of the
barrel and is collected in the collector. The total prepared mix was circulated by using the
procedure described above three to four times to assure thorough mixing. Now die and cone were
bolted to machine. The mix was fed into the hopper. The flywheel was speeded up to 400 rpm
and the clutch was engaged. The extruded brick column was collected in a detachable mould. The
brick column was replaced in the hopper. This procedure was repeated five to ten times until an
uncracked column of uniform length was obtained. Now the experimental set up was ready to
record the observations.
1.4. Experimental observations and Empirical Model [11]
The experimental observations were recorded in tabulated form. As the variables involved were
high in number dimensionless pi terms were evaluated. And an empirical model was generated to
predict the experimental findings. The model was as follows.
Lb / D1 = 0.0043 (LD/D1) -1.8091
*(D12/IgWf) 0.139
*(G) 0.2766
*(√ D1/g. W) 1.27
*(Lc/D1)-1.977
*(P/ D1)1.3075
*(D2 / D1)0.8313
2. IDENTIFICATION OF PROBLEM AND SELECTED APPROACH
The plots are drawn to see the prediction of experimental evidences by the traditional empirical
model. The figures 2 to 8 evaluate and compare the results.
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
42
Figure 2: Graph of comparison between experimental observations and equation based prediction for
LD/D1 Vs Lb/D1
Figure 3: Graph of comparison between experimental observations and equation based prediction for
D12
/Ig)Wf Vs Lb / D1
Figure 4: Graph of comparison between experimental observations and equation based prediction for G Vs
Lb/D1
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
43
Figure 5: Graph of comparison between experimental observations nd equation based prediction for √
(D1/g). W Vs Lb/D1
Figure 6: Graph of comparison between experimental observations and equation based prediction for Lc/
D1 Vs Lb/D1
Figure 7: Graph of comparison between experimental observations and equation based prediction for P/ D1
Vs Lb/D1
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
44
Figure 8: Graph of comparison between experimental observations and equation based prediction for
D2/D1 Vs Lb/D1
Figures 2 to 8 clearly shows that the equation is not able to draw a continuous path through the
experimental findings. As the previous equation derived stand no more to predict the desired
experimental findings, it is forced to go for such a model which will be more reliable and
realistic. The percentage error is of the order of 200 to 300%. In view of the fact that independent
variables involved are high in numbers, it becomes a very tedious and inaccurate work to build an
accurate mathematical model. ANN i.e. Artificial Neural Network has shown its strength in the
field of learning and prediction of the desired results when the input variables are high in numbers
[7]. Since the equation is not predicting the observed data correctly we cannot rely on the same
for predicting the output for the unseen data. On the contrary, ANN model can give more reliable
model for the same.
3. MODIFICATION IN EXISTING DATABASE
The experimental evidences developed during experimentation were very little in number. As a
result experimental database was found to be insufficient for training and validation of the model
generated though ANN simulation.
In order to develop ANN model, the existing database was modified and improved in magnitude
by manoeuvring plots on the basis of present experimental evidences. The intermediate positions
in the plot are positioned and noted [6]. This database generated is as follows.
Table 2. Modified Data
Sr.
No.
Independent Variables Dependent
Variables
LD/D1 D12/Ig.Wf G √(D1/g).W Lc/
D1
P/
D1
D2 / D1 Lb / D1
1 0.2 3.7 4.5 9.19 0.5 0.24 0.4 1.174
↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓
240 0.5 2.102 4.5 9.19 0.5 0.24 0.4 0.854
↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓
550 0.5 3.7 2.867 9.19 0.5 0.24 0.4 1.455
↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓
710 0.5 3.7 4.5 2.841 0.5 0.24 0.4 0.203
↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓
912 0.5 3.7 4.5 9.19 0.4391 0.24 0.4 0.995
↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓
1555 0.5 3.7 4.5 9.19 0.5 0.24 0.39795 1.157
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
45
4. FORMULATION AND IMPLEMENTATION OF SEQUENTIAL MODELLING
EVALUATION
Modelling a system through ANN simulation involves use of ANN parameters appropriately. A
topology is nothing but the complete architecture of network formed through the use of ANN
parameters [9]. The ANN parameters should be varied systematically in an attempt to identify
best topology for a specified problem. The number of layers was restricted to two as the variables
involved were high in number. A table for evaluation of modelling technique is formed as below
[5]. The shaded column indicates the variation of that particular parameter and shaded row shows
the slandered value of that parameter.
Table 3. Table of sequential modelling evaluation
Program
Number
Hidden
layer
Size
Type of
Training
Function
Performance
Function
Types of transfer
function Type of
Learning
AlgorithmLayer1 Layer2
P1 20 trainlm mse logsig purelin learngd
P2 100 trainlm mse logsig purelin learngd
P3 200 trainlm mse logsig purelin learngd
P4 100 trainb mse logsig purelin learngd
P5 100 trainbfg mse logsig purelin learngd
P6 100 trainbr mse logsig purelin learngd
P7 100 trainc mse logsig purelin learngd
P8 100 trainlm mae logsig purelin learngd
P9 100 trainlm sse logsig purelin learngd
P10 100 trainlm sse tansig purelin learngd
P11 100 trainlm sse logsig purelin learngd
P12 100 trainlm sse logsig hardlim learngd
P13 100 trainlm sse logsig tansig learngd
P14 100 trainlm sse tansig logsig learngd
P15 100 trainlm sse tansig satlin learngd
P16 100 trainlm sse logsig satlin learngd
P17 100 trainlm sse logsig poslin learngd
P18 100 trainlm sse logsig tansig learncon
P19 100 trainlm sse logsig tansig learngd
P20 100 trainlm sse logsig tansig learnh
P21 100 trainlm sse logsig tansig learnk
The ANN parameters like hidden layer size, Training algorithm, performance function, transfer
functions of layers, learning Algorithm are decided to vary in order to see its effect over the
predication of model. Every parameter posses its diversified standard values out of which some
are chosen and their effects are observed after and during training. The table 3 shows the program
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
46
number and respected value of each parameter. For each case of a program one parameter is
varied and other parameters were allocated some constant standard value.
The training for all programs are carried and results were plotted to see the outcome. The training
with so many parameters gives fantastic diversified results which are presented in graphical form
as follows.
5. GRAPHICAL REPRESENTATION OF RESULTS AFTER TRAINING
Figure 9: Neural response with 20 Neurons
Figure 10: Percentage error with 20 neurons
Figure 11: Neural response with 100 Neurons
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
47
Figure 12: Percentage error with 100 Neurons
Figure 13: Neural response with 200 Neurons
Figure 14: Percentage error with 200 Neurons
Figure 15: Neural response with training Function “trainb”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
48
Figure 16: Percentage error with training Function “trainb”
Figure 17: Neural response with training Function “trainbfg”
Figure 18: Percentage error with training Function “trainbfg”
Figure 19: Neural response with training Function “trainbr”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
49
Figure 20: Percentage error with training Function “trainbr”
Figure 21: Neural response with training Function “trainc”
Figure 22: Percentage error with training Function trainc”
Figure 23: Neural response with performance Function “mae”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
50
Figure 24: Percentage error with performance Function “mae”
Figure 25: Neural response with performance Function “sse”
Figure 26: Percentage error with performance Function “sse”
Figure 27: Neural response with layer transfer Function “tansig, purelin”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
51
Figure 28: Percentage error with layer transfer Function “tansig, purelin”
Figure 29: Neural response with layer transfer Function “logsig, purelin”
Figure 30: Percentage error with layer transfer Function “logsig, purelin”
Figure 31: Neural response with layer transfer Function “logsig, hardlim”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
52
Figure 32: Percentage error with layer transfer Function “logsig, hardlim”
Figure 33: Neural response with layer transfer Function “logsig, tansig”
Figure 34: Percentage error with layer transfer Function “logsig, tansig”
Figure 35: Neural response with layer transfer Function “tansig, logsig”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
53
Figure 36: Percentage error with layer transfer Function “tansig, logsig”
Figure 37: Neural response with layer transfer Function “tansig, satlin”
Figure 38: Percentage error with layer transfer Function “tansig, satlin”
Figure 39: Neural response with layer transfer Function “tansig, purlin”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
54
Figure 40: Percentage error with layer transfer Function “tansig, purlin”
Figure 41: Neural response with layer transfer Function “logsig, poslin”
Figure 42: Percentage error with transfer Function “logsig, poslin”
Figure 43: Neural response with Learn Function “learncon”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
55
Figure 44: Percentage error with Learn Function “learncon”
Figure 45: Neural response with Learn Function “learngd”
Figure 46: Percentage error with Learn Function “learngd”
Figure 47: Neural response with Learn Function “learnh”
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
56
Figure 48: Percentage error with Learn Function “learnh”
Figure 49: Neural response with Learn Function “learnk”
Figure 50: Percentage error with Learn Function “learnk”
6. DISCUSSION OF RESULTS AFTER TRAINING
6.1 Effect of variation of number of neuron in hidden layer
 Figure 8 to 10 shows that increase of number of neuron gives better prediction.
 But as the number goes to 200 it takes very large time to train the network
 Hence Layer size is limited to 100.
6.2 Effect of variation training styles
 Figure 10 to 14 gives the results when training styles are changed.
 The results are too bad with “trainb” & “trainc”
 As a result it can be concluded that training styles affect the performance of network to
great extent.
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
57
 It is been observed that back propagation training functions are better for fitting function
and the performance seems superior with “trainlm”
6.3 Effect of variation of Performance Function
 Figure 14 to 16 displays the results with change of performance function
 The change of performance function has shown little effect on prediction
 Performance function “sse” has shown better results.
6.4 Effect of variation transfer function to hidden layer
 Figure 16 to 24 shows the outcome when transfer function to hidden layers was changed.
 There are too many transfer functions to use and network has two hidden layers. Hence
various combinations of these transfer functions were use to see the effect on
performance.
 It is been observed that the outer most layer with linear transfer function “purelin” gives
better results
 The combination of “logsig, tansig” transfer functions is found best for this case whereas
“with “tansig, logsig” is worst.
6.5 Effect of variation of Learning Function
 Figure 24 to 28 put on view the results with variation of learning function.
 It clearly shows the is very mild effect of variation learning function on performance of
network
 Out of those learning functions “learncon” & “traingd” were very closed
 “learngd” is selected amongst them.
7. CONCLUSION
 The ANN simulation carried for HPFM operated Brick Making M/C gives satisfactory
results
 The simulation is carried out is much exhaustive
 It includes almost all ANN parameters to see its effect on network performance
 The error in neural prediction much smaller and of the average of 5-10 %
8. FUTURE SCOPE
 Prediction of ANN model may be compared with the available empirical model.
 The best ANN model may be further used to develop another mathematical model.
 The ANN model could be validated through unseen data.
 This mathematical model then could be utilized to develop a physical controller.
International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013
58
REFERENCES
[1] Modak J. P. and Askhedkar R. D. “Hypothesis for the extrusion of lime flash sand brick using a
manually driven Brick making machine”, Bulding Research and Information U.K., V22,NI, Pp 47-
54, 1994
[2] Modak J. P. and Bapat A. R. “Manually driven flywheel motor operates wood turning machine”,
Contepory Ergonomics, Proc. Ergonomics Society annual convension13-16April, Edinburg,
Scotland, Pp 352-357, 1993.
[3] Sohoni V. V., Aware H. V. and Modak J. P. “ Manual Manufacture of Keyed Bricks”, Building
Research and Information UK, Vol 25, N6, 1997, 354-364.
[4] Modak J. P.”Design and Development of Manually Energized Process Machines having
Relevance to Village/Agriculture and other productive operations, Application of manually
energized flywheel motor for cutting of wood strip”, Human Power, send for Publications.
[5] H. Schenck Junior “Theory of Engineering Experimentation”, MC Graw Hill, New York.
[6] P. A. Chandak, “Modelling of manually driven brick making machine by use of ANN”, M. Tech.
Thesis, PCE, Nagpur
[7]. S. N. Shvanandam, “Introduction to Neural Network using Matlab 6.0”, McGraw Hill publisher.
[8] Stamtios V. Kartaplopoulos , Understanding Neural Networks and Fuzzy Logics, IEEE Press
[9] Neural Network Toolbox TM
7 User’s Guide R2010a, , Mathworks.com.
[10] Rudra Prtap, “Getting Started with Matlab7,” Oxford, First Indian Edition 2006.
[11] A. R. Bapat, “Experimental Optimization of a manually driven flywheel motor”, M.E. Thesis,
VNIT, Nagpur.
[12] A. R. Bapat, Experimentation of Generalized experimental model for a manually driven flywheel
motor”, PhD Thesis, VNIT, Nagpur.
Authors
Pawan A. Chandak, Asstt Professor, Mechanical Engg, DMIETR, Wardha (MH), India
,Specilization: Artificial Neural Networks, Design and Fabrication, Vibration based
predictive Maintenance.

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OPTIMIZATION OF ARTIFICIAL NEURAL NETWORK MODEL FOR IMPROVEMENT OF ARTIFICIAL INTELLIGENCE OF MANUALLY DRIVEN BRICK MAKING MACHINE POWERED BY HPFM

  • 1. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 DOI : 10.5121/ijccms.2013.2304 39 OPTIMIZATION OF ARTIFICIAL NEURAL NETWORK MODEL FOR IMPROVEMENT OF ARTIFICIAL INTELLIGENCE OF MANUALLY DRIVEN BRICK MAKING MACHINE POWERED BY HPFM P. A. Chandak1 and J. P. Modak2 1 Department of Mechanical Engineering, DMIETR, Wardha (MH), India 2 Professor Emeritus, Dean (R&D), PCE, Nagpur(MH), India ABSTRACT Considerable development has been done by some authors of this paper towards development of manufacturing process units energized by Human Powered Flywheel Motor (HPFM) as an energy source. This machine system comprises three sub systems namely (i) HPFM (ii) Torsionally Flexible Clutch (TFC) (iii) A Process Unit. Process unit so far tried are mostly rural based such as brick making machine (both rectangular and keyed cross sectioned), Low head water lifting, Wood turning, Wood strips cutting, etc HPFM comprises pedalling system similar to bicycle, a speed rising gear pair and a flywheel big enough such that a young lad of 21-25 years, 165cm height, slim structure can pump energy around 30,000 N-m in minutes time. Once such an energy is stored peddling is stopped and a special type of TFC is engaged which very efficiently brings about momentum and energy transfer from flywheel to a process unit. Process unit utilization time upon clutch engagement is 5 to 15 seconds depending on the application. In other word process units needing power of order of 3 hp to 10 hp can be powered by such a machine concept. Experimental data base model is formulated for Human Powered Flywheel Motor Energized Brick Making Machine (HPFMEBMM). The focus of the present paper is on development of an optimum Artificial Neural Network (ANN) model which will predict the experimental evidences accurately and precisely. The optimisation is acknowledged though variation of various parameters of ANN topology like training algorithm, learning algorithm, size of hidden layer, number of hidden layers, etc while training the network and accepting the best value of that parameter. The paper also discusses the effects and results of variation of various parameters on prediction of network. KEYWORDS ANN, Matlab, Manually driven brick making machine. Simulation. 1. REVIEW OF THE BRICK MAKING MACHINE AND ITS PROCESS UNIT 1.1 Working of manually driven Brick making machine A manually driven Auger-type brick making [1][3] machine developed by Dr. J. P. Modak is as shown in figure. The operator drives the flywheel (17) though chain (25) and a pair of gears (19, 20). The chain drive is utilized for first stage transmission because the drive is required to be irreversible. This is achieved with the conventional bicycle drive with a free wheel (21). When the flywheel attains sufficient speed, the single jaw clutch (13, 15) is engaged. The clutch drives the auger screw through a pair of gears (9, 10). The mix fed through hopper (3). A cone (2) connects the drum (30) to the die (1). The cone eliminates the rotary motion of the mix before it
  • 2. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 40 enters the die. The extracted column is collected in a detachable mould (4). It is lined on the inside by Perspex to provide least resistance to motion of the column. The column is subsequently demoulded by placing it upside down on the platform. The mould is moved horizontally, leaving the column on the platform. About one or two hours after the column is laid on the platform, it becomes stiff enough to be cut by a cutter to form bricks of standard size. 1.DIE, 2.CONE, 3.HOPPER, 4.AL MOULD, 5.MOULDING STAND, 6.CONVEYOR SCREW, 7.CONVEYER SHAFT, 8.HOPPER, 9. GEAR, 10.PINION, 11.PINION SHAFT, 12.BEARING, MOVABLE HALF CLUTCH, 14.CLUTCH LEVER, 15.FIXED HALF CLUTCH, 16.FLYWHEEL SHAFT, 17.FLYWHEEL, 18, BEARING FOR FLYWHEEL, 19.PINION II, 20.GEAR II, 21.FREWHELL, 22.INTERMEDIATE SHAFT, 23.BEARING FOR INTERMEDIATE SHAFT, 24.CRANK GEAR, 25.PINION FOLLOWER CHAIN, 26.DRIVER SEAT, 27.HANDLE, 28.BRACKET, 29.FRAME, 30.CONVEYOR DRUM. Figure 1. Manually driven Brick Making Machine The following process variables were involved in the process of experimentation. [1] Table 1. Process variables and their dimensions Sr No. Description of variables Type of variable Symbol Dimension 1 Weight of lime Independent WL ML-1T-2 2 Weight of sand Independent Ws ML-1T-2 3 Weight of flyash Independent Wf ML-1T-2 4 Weight of water Independent Ww ML-1T-2 5 Outside diameter of screw Independent D1 L 6 Inside diameter of screw Independent D2 L 7 Pitch of Screw Independent P L 8 Larger Diameter of Cone Independent D1 L 9 Smaller Diameter of Cone Independent D3 L 10 Length of cone Independent LC L 11 Length of die Independent LD L 12 Moment of Inertia of flywheel Independent I ML2 13 Angular velocity of flywheel Independent W T-1
  • 3. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 41 14 Acceleration of due to gravity Independent G LT-2 15 Gear ratio Independent G - 16 Length of square side of die Independent S L 17 Strength of brick Dependent Sb ML-1T-2 18 Length of Extruded Brick Column Dependent Lb L 19 Time of Extrusion Dependent Te T 20 Maximum length of Extruded Brick Column Dependent Lbm L 21 Critical Pressure of Extrusion Dependent Pc ML-1T-2 22 Instantaneous Torque on the angular shaft Dependent T ML-1T-2 1.2. Experimental setup The experimental setup [1] basically consists of a manually driven brick making machine with following facilities  Facility to change die, cone, auger, screw, blades and gears  Facility to mount the torque meter and to record process torque during extrusion process.  Facility to mount technogerators to record speeds of flywheel and auger screw. 1.3. Procedure of Experimentation Initially the machine parameters were set as per the plan of experimentation. A homogeneous mix of lime-flyash-sand, in requisite proportion by weight, was prepared by adding suitable amount of water. The mix was soaked for 48 hours and was kept ready for use. To assure thorough mixing, die and cone machine were removed. Sufficient mix was fed into the hopper. The flywheel was speeded up to 400 rpm and the clutch was engaged. The mix passes out of the barrel and is collected in the collector. The total prepared mix was circulated by using the procedure described above three to four times to assure thorough mixing. Now die and cone were bolted to machine. The mix was fed into the hopper. The flywheel was speeded up to 400 rpm and the clutch was engaged. The extruded brick column was collected in a detachable mould. The brick column was replaced in the hopper. This procedure was repeated five to ten times until an uncracked column of uniform length was obtained. Now the experimental set up was ready to record the observations. 1.4. Experimental observations and Empirical Model [11] The experimental observations were recorded in tabulated form. As the variables involved were high in number dimensionless pi terms were evaluated. And an empirical model was generated to predict the experimental findings. The model was as follows. Lb / D1 = 0.0043 (LD/D1) -1.8091 *(D12/IgWf) 0.139 *(G) 0.2766 *(√ D1/g. W) 1.27 *(Lc/D1)-1.977 *(P/ D1)1.3075 *(D2 / D1)0.8313 2. IDENTIFICATION OF PROBLEM AND SELECTED APPROACH The plots are drawn to see the prediction of experimental evidences by the traditional empirical model. The figures 2 to 8 evaluate and compare the results.
  • 4. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 42 Figure 2: Graph of comparison between experimental observations and equation based prediction for LD/D1 Vs Lb/D1 Figure 3: Graph of comparison between experimental observations and equation based prediction for D12 /Ig)Wf Vs Lb / D1 Figure 4: Graph of comparison between experimental observations and equation based prediction for G Vs Lb/D1
  • 5. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 43 Figure 5: Graph of comparison between experimental observations nd equation based prediction for √ (D1/g). W Vs Lb/D1 Figure 6: Graph of comparison between experimental observations and equation based prediction for Lc/ D1 Vs Lb/D1 Figure 7: Graph of comparison between experimental observations and equation based prediction for P/ D1 Vs Lb/D1
  • 6. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 44 Figure 8: Graph of comparison between experimental observations and equation based prediction for D2/D1 Vs Lb/D1 Figures 2 to 8 clearly shows that the equation is not able to draw a continuous path through the experimental findings. As the previous equation derived stand no more to predict the desired experimental findings, it is forced to go for such a model which will be more reliable and realistic. The percentage error is of the order of 200 to 300%. In view of the fact that independent variables involved are high in numbers, it becomes a very tedious and inaccurate work to build an accurate mathematical model. ANN i.e. Artificial Neural Network has shown its strength in the field of learning and prediction of the desired results when the input variables are high in numbers [7]. Since the equation is not predicting the observed data correctly we cannot rely on the same for predicting the output for the unseen data. On the contrary, ANN model can give more reliable model for the same. 3. MODIFICATION IN EXISTING DATABASE The experimental evidences developed during experimentation were very little in number. As a result experimental database was found to be insufficient for training and validation of the model generated though ANN simulation. In order to develop ANN model, the existing database was modified and improved in magnitude by manoeuvring plots on the basis of present experimental evidences. The intermediate positions in the plot are positioned and noted [6]. This database generated is as follows. Table 2. Modified Data Sr. No. Independent Variables Dependent Variables LD/D1 D12/Ig.Wf G √(D1/g).W Lc/ D1 P/ D1 D2 / D1 Lb / D1 1 0.2 3.7 4.5 9.19 0.5 0.24 0.4 1.174 ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ 240 0.5 2.102 4.5 9.19 0.5 0.24 0.4 0.854 ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ 550 0.5 3.7 2.867 9.19 0.5 0.24 0.4 1.455 ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ 710 0.5 3.7 4.5 2.841 0.5 0.24 0.4 0.203 ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ 912 0.5 3.7 4.5 9.19 0.4391 0.24 0.4 0.995 ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ ↓ 1555 0.5 3.7 4.5 9.19 0.5 0.24 0.39795 1.157
  • 7. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 45 4. FORMULATION AND IMPLEMENTATION OF SEQUENTIAL MODELLING EVALUATION Modelling a system through ANN simulation involves use of ANN parameters appropriately. A topology is nothing but the complete architecture of network formed through the use of ANN parameters [9]. The ANN parameters should be varied systematically in an attempt to identify best topology for a specified problem. The number of layers was restricted to two as the variables involved were high in number. A table for evaluation of modelling technique is formed as below [5]. The shaded column indicates the variation of that particular parameter and shaded row shows the slandered value of that parameter. Table 3. Table of sequential modelling evaluation Program Number Hidden layer Size Type of Training Function Performance Function Types of transfer function Type of Learning AlgorithmLayer1 Layer2 P1 20 trainlm mse logsig purelin learngd P2 100 trainlm mse logsig purelin learngd P3 200 trainlm mse logsig purelin learngd P4 100 trainb mse logsig purelin learngd P5 100 trainbfg mse logsig purelin learngd P6 100 trainbr mse logsig purelin learngd P7 100 trainc mse logsig purelin learngd P8 100 trainlm mae logsig purelin learngd P9 100 trainlm sse logsig purelin learngd P10 100 trainlm sse tansig purelin learngd P11 100 trainlm sse logsig purelin learngd P12 100 trainlm sse logsig hardlim learngd P13 100 trainlm sse logsig tansig learngd P14 100 trainlm sse tansig logsig learngd P15 100 trainlm sse tansig satlin learngd P16 100 trainlm sse logsig satlin learngd P17 100 trainlm sse logsig poslin learngd P18 100 trainlm sse logsig tansig learncon P19 100 trainlm sse logsig tansig learngd P20 100 trainlm sse logsig tansig learnh P21 100 trainlm sse logsig tansig learnk The ANN parameters like hidden layer size, Training algorithm, performance function, transfer functions of layers, learning Algorithm are decided to vary in order to see its effect over the predication of model. Every parameter posses its diversified standard values out of which some are chosen and their effects are observed after and during training. The table 3 shows the program
  • 8. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 46 number and respected value of each parameter. For each case of a program one parameter is varied and other parameters were allocated some constant standard value. The training for all programs are carried and results were plotted to see the outcome. The training with so many parameters gives fantastic diversified results which are presented in graphical form as follows. 5. GRAPHICAL REPRESENTATION OF RESULTS AFTER TRAINING Figure 9: Neural response with 20 Neurons Figure 10: Percentage error with 20 neurons Figure 11: Neural response with 100 Neurons
  • 9. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 47 Figure 12: Percentage error with 100 Neurons Figure 13: Neural response with 200 Neurons Figure 14: Percentage error with 200 Neurons Figure 15: Neural response with training Function “trainb”
  • 10. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 48 Figure 16: Percentage error with training Function “trainb” Figure 17: Neural response with training Function “trainbfg” Figure 18: Percentage error with training Function “trainbfg” Figure 19: Neural response with training Function “trainbr”
  • 11. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 49 Figure 20: Percentage error with training Function “trainbr” Figure 21: Neural response with training Function “trainc” Figure 22: Percentage error with training Function trainc” Figure 23: Neural response with performance Function “mae”
  • 12. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 50 Figure 24: Percentage error with performance Function “mae” Figure 25: Neural response with performance Function “sse” Figure 26: Percentage error with performance Function “sse” Figure 27: Neural response with layer transfer Function “tansig, purelin”
  • 13. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 51 Figure 28: Percentage error with layer transfer Function “tansig, purelin” Figure 29: Neural response with layer transfer Function “logsig, purelin” Figure 30: Percentage error with layer transfer Function “logsig, purelin” Figure 31: Neural response with layer transfer Function “logsig, hardlim”
  • 14. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 52 Figure 32: Percentage error with layer transfer Function “logsig, hardlim” Figure 33: Neural response with layer transfer Function “logsig, tansig” Figure 34: Percentage error with layer transfer Function “logsig, tansig” Figure 35: Neural response with layer transfer Function “tansig, logsig”
  • 15. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 53 Figure 36: Percentage error with layer transfer Function “tansig, logsig” Figure 37: Neural response with layer transfer Function “tansig, satlin” Figure 38: Percentage error with layer transfer Function “tansig, satlin” Figure 39: Neural response with layer transfer Function “tansig, purlin”
  • 16. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 54 Figure 40: Percentage error with layer transfer Function “tansig, purlin” Figure 41: Neural response with layer transfer Function “logsig, poslin” Figure 42: Percentage error with transfer Function “logsig, poslin” Figure 43: Neural response with Learn Function “learncon”
  • 17. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 55 Figure 44: Percentage error with Learn Function “learncon” Figure 45: Neural response with Learn Function “learngd” Figure 46: Percentage error with Learn Function “learngd” Figure 47: Neural response with Learn Function “learnh”
  • 18. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 56 Figure 48: Percentage error with Learn Function “learnh” Figure 49: Neural response with Learn Function “learnk” Figure 50: Percentage error with Learn Function “learnk” 6. DISCUSSION OF RESULTS AFTER TRAINING 6.1 Effect of variation of number of neuron in hidden layer  Figure 8 to 10 shows that increase of number of neuron gives better prediction.  But as the number goes to 200 it takes very large time to train the network  Hence Layer size is limited to 100. 6.2 Effect of variation training styles  Figure 10 to 14 gives the results when training styles are changed.  The results are too bad with “trainb” & “trainc”  As a result it can be concluded that training styles affect the performance of network to great extent.
  • 19. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 57  It is been observed that back propagation training functions are better for fitting function and the performance seems superior with “trainlm” 6.3 Effect of variation of Performance Function  Figure 14 to 16 displays the results with change of performance function  The change of performance function has shown little effect on prediction  Performance function “sse” has shown better results. 6.4 Effect of variation transfer function to hidden layer  Figure 16 to 24 shows the outcome when transfer function to hidden layers was changed.  There are too many transfer functions to use and network has two hidden layers. Hence various combinations of these transfer functions were use to see the effect on performance.  It is been observed that the outer most layer with linear transfer function “purelin” gives better results  The combination of “logsig, tansig” transfer functions is found best for this case whereas “with “tansig, logsig” is worst. 6.5 Effect of variation of Learning Function  Figure 24 to 28 put on view the results with variation of learning function.  It clearly shows the is very mild effect of variation learning function on performance of network  Out of those learning functions “learncon” & “traingd” were very closed  “learngd” is selected amongst them. 7. CONCLUSION  The ANN simulation carried for HPFM operated Brick Making M/C gives satisfactory results  The simulation is carried out is much exhaustive  It includes almost all ANN parameters to see its effect on network performance  The error in neural prediction much smaller and of the average of 5-10 % 8. FUTURE SCOPE  Prediction of ANN model may be compared with the available empirical model.  The best ANN model may be further used to develop another mathematical model.  The ANN model could be validated through unseen data.  This mathematical model then could be utilized to develop a physical controller.
  • 20. International Journal of Chaos, Control, Modelling and Simulation (IJCCMS) Vol.2, No.3, September 2013 58 REFERENCES [1] Modak J. P. and Askhedkar R. D. “Hypothesis for the extrusion of lime flash sand brick using a manually driven Brick making machine”, Bulding Research and Information U.K., V22,NI, Pp 47- 54, 1994 [2] Modak J. P. and Bapat A. R. “Manually driven flywheel motor operates wood turning machine”, Contepory Ergonomics, Proc. Ergonomics Society annual convension13-16April, Edinburg, Scotland, Pp 352-357, 1993. [3] Sohoni V. V., Aware H. V. and Modak J. P. “ Manual Manufacture of Keyed Bricks”, Building Research and Information UK, Vol 25, N6, 1997, 354-364. [4] Modak J. P.”Design and Development of Manually Energized Process Machines having Relevance to Village/Agriculture and other productive operations, Application of manually energized flywheel motor for cutting of wood strip”, Human Power, send for Publications. [5] H. Schenck Junior “Theory of Engineering Experimentation”, MC Graw Hill, New York. [6] P. A. Chandak, “Modelling of manually driven brick making machine by use of ANN”, M. Tech. Thesis, PCE, Nagpur [7]. S. N. Shvanandam, “Introduction to Neural Network using Matlab 6.0”, McGraw Hill publisher. [8] Stamtios V. Kartaplopoulos , Understanding Neural Networks and Fuzzy Logics, IEEE Press [9] Neural Network Toolbox TM 7 User’s Guide R2010a, , Mathworks.com. [10] Rudra Prtap, “Getting Started with Matlab7,” Oxford, First Indian Edition 2006. [11] A. R. Bapat, “Experimental Optimization of a manually driven flywheel motor”, M.E. Thesis, VNIT, Nagpur. [12] A. R. Bapat, Experimentation of Generalized experimental model for a manually driven flywheel motor”, PhD Thesis, VNIT, Nagpur. Authors Pawan A. Chandak, Asstt Professor, Mechanical Engg, DMIETR, Wardha (MH), India ,Specilization: Artificial Neural Networks, Design and Fabrication, Vibration based predictive Maintenance.