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U. V. Mangudkar et al Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303

RESEARCH ARTICLE

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OPEN ACCESS

Formability Analysis and Its Parameters –A Review Paper
U. V. Mangudkar*, Dr. R. B. Hiremath**
*

PG Student, WIT,Solapur
Professor of Mechanical Enginnering WIT,Solapur

**

ABSTRACT
This paper represents review of parameters which affects sheet metal formability and also about forming limit
diagram (FLD).The parameters are punch nose radius, blank temperature, die arc radius, punch velocity, blank
holding force(BHF),blank shape, spring back etc. The first section of paper represents about formability. Second
section reviews different parameters that affect sheet metal forming. Section 3 explains that formability of sheet
metal defined in terms of two dimensional strain maps. It also describes state of strain measures formability. It
deals with different research work dealing with forming limit diagram (FLD). The forming limit diagram (FLD)
gives an indication whether the material can sustain certain ratio of strains without failing is of great help.
Keywords:- BHF,FLD,Sheet metal formability.

I.

INTRODUCTION

The forming of metals into desired shapes is
almost the oldest fabricating technique. Metal
forming is an economical method of manufacturing
components because loss of material is too less. It is a
process in which the desired shapes and size of
components are obtained through the plastic
deformation of metal. Sheet metals are widely used
for industrial and consumer parts because of its
capacity for being bent and formed into intricate
shapes. Sheet metal parts comprise a large fraction of
automotive, agricultural machinery, and aircraft
components as well as consumer appliances.

II.

FORMING PARAMETERS

Successful sheet metal forming operation
depends on the selection of punch nose radius, die arc
radius, punch velocity, blank holding force, spring
back, blank size and shape, die clearance and
lubrication. Forming limit diagram (FLD) and circle
grid analysis helps to understand forming in sheet
metals. The summary of some of the works conducted
by different researchers regarding forming is listed
below; they described the analytical approach and
experimental results.
2.1 Punch nose radius
Dr.Waleed K.Jawad ,Jamal H.Mohamed[1]
studied the effect of punch nose radius on deep
drawing operation. In this work, six types of punches
with various nose radii have been used to form a
cylindrical cup of (44mm) outer diameter,(28mm)
height, and(0.5mm)sheet thickness of mild steel of
(0.15%) carbon content. A commercially finite
element program code (ANSYS 5.4), was used to
perform the numerical simulation of the deep drawing
operation, and the numerical results were compared
with the experimental work. The results show that,
the value of work required to form parts with large
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nose radii is much more than the value required to
form parts with small punch nose radii. The greatest
thinning is seen to occur with hemispherical punch
(Dome shaped punch) due to great stretching of the
metal over the punch head. The maximum tensile
stresses and the maximum thinning of the dome wall
occur nearly at the apex of the dome.
2.2 Blank temperature
G. Venkateswarlu, M. J. Davidson and G. R.
N. Tagore[2] extensively studied formability aspects
of aluminium 7075 to develop useful components of
complex shapes. In that study, the significance of
three important deep drawing process parameters
namely blank temperature, die arc radius and punch
velocity on the deep drawing characteristics of
aluminium 7075 sheet was determined. The
combination of finite element method and Taguchi
analysis was used to determine the influence of
process parameters. Simulations were carried out as
per orthogonal array using DEFORM 2Dsoftware.
Based on the predicted deformation of deep drawn
cup and analysis of variance test (Anova), it was
observed that blank temperature has greatest
influence on the formability of aluminium material
followed by punch velocity and die arc radius.
2.3 Blank holding force
Y. Marumo, H. Saiki, L Ruan [3] has carried
out the study regarding variation in the blank holding
force required for the elimination of wrinkling and the
limiting drawing ratio with sheet thickness. They
found that blank holding force required for the
elimination of wrinkling increased rapidly as the sheet
thickness decreased. When the sheet thickness was
very thin, the blank holding force was strongly
influenced by the coefficient of friction. The limiting
drawing ratio decreased as sheet thickness decreased
and it decreased rapidly below 0.04 mm thickness.
300 | P a g e
U. V. Mangudkar et al Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303
When the sheet thickness was very thin, the limiting
drawing ratio was strongly influenced by the
coefficient of friction.
2.4 Intital blank shape
M. Ahmetoglu, T. R. Broek, G. Kinzel, T.
Altan [4] have carried out the study of effect of
process parameters such as initial blank shape and the
blank holding force on the final part quality (i.e.,
wrinkling and fracture). During the initial
experiments, it was found that the oval blank shape
had the worst formability, from a fracture point of
view, among the three blank shapes (i.e., oval,
oblong, and rectangle). The oval shape reduced the
fracture limit of AA 2008-T4. However, it caused
smaller wrinkling heights in the flange along the sides
of the rectangular pan. Control of the (BHF) as a
function of time improves the formability and the
quality of the final part. However, BHF control in
time is not enough by itself. Since the deformation
characteristics are not uniform around the periphery
of the rectangle, the BHF has to be controlled as a
function of location, too. Metal flow can be controlled
by using draw beads on the sides of the rectangle.
2.5 An optimization strategy for the blank holder
force (BHF)
H. Gharib, A.S. Wifi, M. Younan, A. Nassef
[5] have proposed an optimization strategy for the
blank holder force (BHF) which searches for the BHF
scheme that minimizes the maximum punch force and
avoids process limits. That strategy was applied to the
linearly varying BHF scheme and compared to the
constant BHF. They found that the optimized linear
BHF scheme resulted in an improved cup forming
when compared to that produced by the constant BHF
scheme. The BHF scheme is optimized for different
cases of drawing ratios and die coefficients of friction
in order to analyze the nature of the optimum linear
BHF scheme. It was found that the slope of the linear
BHF scheme increases with the increase in the
drawing ratio in a linear manner. Also, the intercept
of the function showed a nearly linear variation with
the drawing ratio. A general equation is deduced for
the optimum blank holder force at any drawing ratio
for the cup under study.
2.6 Spring back
W.M. Chan, H.I. Chew, H.P. Lee, B.T.
Cheok [6] have presented a study of spring-back in
the V-bending metal forming process with one
clamped end and one free end. They found that
spring-back occurs at the die-lip and V-region of the
die model. Different die punch parameters such as
punch radius, punch angle and die-lip radius were
varied to study their effect on spring-back. Also, the
effect of the punch displacement on spring-back was
investigated. The H-convergence test was done to
justify the number of elements used. Softwares used
are Patran, Abaqus/Standard and Abaqus/CAE. Patran
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was used to model the nodes of the sheet metal and
rigid surfaces of the die, pad and punch.
Abaqus/Standard is used to simulate the punching
process. The results were analyzed using
Abaqus/CAE. Their analysis shows that spring-back
angle of the valley region decreased with increment
of punch radius and punch angle and spring-back is
dependent on punch radius, punch angle and die-lip
radius.

III.

FORMING LIMIT DIAGRAM

The forming limit diagram (FLD) (Fig.3.1)
gives an indication whether the material can sustain
certain ratio of strains without failing is of great help.
Keeler[7] pioneered the application of forming limit
diagrams (FLD) for accessing the formability of sheet
metal.

Fig.3.1 Forming limit diagram[8]
Many researchers have tried to determine the
FLD diagrams for different sheet metals commonly
used in forming operations either experimentally or
theoretically. The experimental method consists of
printing a grid pattern of circles of appropriate
diameter (generally 2 mm to 4 mm) on the surface of
sheet. The sheet is deformed as required but in stages.
After each stage the grid pattern is examined. The
advantage of printing circular grids is that during the
deformation the circles will get deformed into ellipse
with major and minor axes directed along the
principal directions of strain. The measurement of the
axes and knowing the original diameter we can
determine principal strains and their directions. As the
forming progresses, at some region neck formation
may occur. The ratio of strains is determined at the
region. This is a point on FLD diagram or curve
which separates the safe and unsafe regions.
In 1967, Marciniak and Kuczynski proposed
their analytical model for limit-strain prediction based
on the initial in homogeneity of a material, which has
been foundational for much of the subsequent work in
this area and is commonly referred to as theM–K
theory [9]. They attributed changes in limiting strain
values to the loading history of the specimen, the ratio
of the principal stresses, and several material
301 | P a g e
U. V. Mangudkar et al Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303
properties, including the initial in homogeneity. They
noted that the largest limiting strains in the biaxial
stretching region were obtained during equal biaxial
tension, whilst the minimum values occurred in
plane-strain.One of the primary applications of the
circular grid system and FLD proposed by Keeler was
the analysis of strain distributions in actual stampings
to improve part quality and optimize die design [10].
Since Keeler’s experiments continued to verify his
earlier results, showing that the lowest formability
exists under plane strain conditions, he proposed
restricting the inward flow of metal from the flange in
order to induce biaxial tensile strains, thereby
increasing the forming limits. The preceding studies
focused on the determination of forming limits solely
in the region of biaxial tension. However, in 1968,
Goodwin used a combination ofcup- and tension-tests
to obtain a failure band in both the negative and
positive quadrants of minor strain, creating the
general form of the forming-limit diagram.
In order to reveal the effects of planar
anisotropy on formability, Marciniak et al. performed
an experimental study involving steel, aluminum, and
copper [11]. These tests were performed under
proportional-straining conditions, and showed that the
forming limits were significantly different in the
rolling direction compared with transverse direction.
This demonstrated that the limit curve does not
consist of mirror images which begin at the principal
axes and meet at the state of equal biaxial tension;
instead, the limit strains are generally somewhat
greater in the rolling direction.
A further investigation of variations in the
forming limit diagram was conducted by Ghosh and
Hecker, who concluded that the limit strains obtained
in punch stretching operations were considerably
higher than those resulting from in-plane stretching
tests [12,13]. Their in-plane stretching tests employed
the use of a polyethylene spacer on either side of the
nose of a punch in order to induce in-plane
deformation. They theorized that the friction and
curvature present during punch stretching cause strain
localization to take place at a much lower rate than
for in-plane stretching. Up to this point, most work on
constructing the forming-limit diagram had employed
the use of grid strain analysis on actual automotive
stampings or on test specimens deformed by punches
of various geometries. In 1975, Hecker introduced a
methodical approach involving the stretching of
sheets of various widths over a hemispherical punch
to obtain strain conditions ranging from uniaxial
tension to balanced biaxial tension[14]. Using the
onset of localized necking to define a single limit of
failure, Hecker obtained a forming-limit curve lying
mostly within the Keeler– Goodwin band. The
advantage of his technique is the ability to determine
an entire forming-limit curve with specimens of
different widths and:or the use of different lubricants.
An analytical model describing neck growth in sheet
metals under various loading conditions, from which
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a predicted forming-limit diagram can be calculated,
was subsequently developed by Lee and Zaverl [15].
Their results corresponded to those of the lower, inplane forming limits. However, the analysis did not
account for the effects of strain history and its
influence on such properties as the plastic strain ratio.

IV.

SUMMARY

The forming limit diagram (FLD) introduced
by Keller and Goodwin probably the most widely
used method for representing sheet metal formability
and extensive literature has been proposed in the last
decade. The forming limit diagram typically
represents the maximum permissible range of major
and minor strains that a typical sheet material can
undertake without failure. The forming limit diagram
is experimentally measured for each sheet material by
placing a grid of circle on the sheet sample and then
deforming the same. A comparison of the original and
the extensions in the marked grids on the sheet
sample provide an estimate of the major and minor
strain of the sample. The permissible range of the
major and minor strains is actually available for a
wide range of sheet metals and used considerably for
designing of deep drawing operations, in particular.
REFERENCES
[1]
Dr.Waleed K.Jawad,Jamal H.Mohamed,
“Studying the Effect of Punch Nose Radius
on
Deep
Drawing
Operation”
Eng.&Tech.Vol.26.No.,pp55-73(2008)
[2]
G. Venkateswarlu, M. J. Davidson and G. R.
N. Tagore, “Influence of process parameters
on the cup drawing of aluminium 7075
sheet” International Journal of Engineering,
Science and Technology Vol. 2, No. 11, pp.
41-49(2010)
[3]
Y. Marumo, H. Saiki, L Ruan , “Effect of
sheet thickness on deep drawing of metal
foils” Journal of Achievements in Materials
and Manufacturing Engineering Vol.20
Issues 1-2 (2007)
[4]
M. Ahmetoglu, T. R. Broek, G. Kinzel, T.
Altan, “Control of Blank Holder Force to
Eliminate Wrinkling and Fracture in DeepDrawing Rectangular Parts” Annals of the
ClRP Vol. 44/1/1995
[5]
H. Gharib, A.S. Wifi, M. Younan, A. Nassef,
“Optimization of the blank holder force in
cup drawing ” Journal of Achievements in
Materials and Manufacturing Engineering,
Volume 18, ISSUE 1-2 September–October
2006
[6]
W.M. Chan, H.I. Chew, H.P. Lee, B.T.
Cheok , “Finite element analysis of springback of V-bending sheet metal forming
processes” Journal of Materials Processing
Technology Vol.148 pp 15–24, (2004)
[7] Keeler, S.P.; Sheet Met.Indust.,Vol.42.
pp.683,1965
302 | P a g e
U. V. Mangudkar et al Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303
[9]

[10]

[11]

[12]

[13]

[14]

[15]

www.ijera.com

Z. Marciniak, K. Kuczynski, “ Limit strains
in the process of stretch-forming sheet
metal” Int. J. Mech. Sci. 9 (1967) 609–620.
S.P. Keeler, “Circular grid system—A
valuable aid for evaluatingsheet metal
formability”
Society
of
Automotive
Engineers Technical Paper No. 680092,
New York, 1968.
Z. Marciniak, K. Kuczynski, T. Pokora, “
Influence of the plastic properties of a
material on the forming limit diagram for
sheet metal in tension” Int. J. Mech. Sci.
15,pp 789–805,1973.
A.K. Ghosh, S.S. Hecker, “Stretching limits
in sheet metals:In-plane versus out-of-plane
deformation” Metall. Trans. 5,pp 2161–
2164,(1974)
S.S. Hecker, “Experimental studies of sheet
stretchability,Formability:
Analysis,
Modeling
and
Experimentation”,
Proceedings October 1977 AIME:ASM
Symposium, “The Metallurgical Society of
the American Institute of Mining,
Metallurgical and Petroleum Engineers” pp.
150–182 New York, 1978,.
S.S. Hecker, “Simple technique for
determining forming limit curves”, Sheet
Met. Ind. 52, pp671–676 (1975).
D. Lee, F. Zaverl Jr., “ Neck growth and
forming limits in sheet metals”, Int. J. Mech.
Sci. 24 (3) pp.157–173(1982).

Books:
[8]
Kalpakjain, Manufacturing Processes for
Engineering Materials ( Pearson Education,
2007 )

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Ax36300303

  • 1. U. V. Mangudkar et al Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303 RESEARCH ARTICLE www.ijera.com OPEN ACCESS Formability Analysis and Its Parameters –A Review Paper U. V. Mangudkar*, Dr. R. B. Hiremath** * PG Student, WIT,Solapur Professor of Mechanical Enginnering WIT,Solapur ** ABSTRACT This paper represents review of parameters which affects sheet metal formability and also about forming limit diagram (FLD).The parameters are punch nose radius, blank temperature, die arc radius, punch velocity, blank holding force(BHF),blank shape, spring back etc. The first section of paper represents about formability. Second section reviews different parameters that affect sheet metal forming. Section 3 explains that formability of sheet metal defined in terms of two dimensional strain maps. It also describes state of strain measures formability. It deals with different research work dealing with forming limit diagram (FLD). The forming limit diagram (FLD) gives an indication whether the material can sustain certain ratio of strains without failing is of great help. Keywords:- BHF,FLD,Sheet metal formability. I. INTRODUCTION The forming of metals into desired shapes is almost the oldest fabricating technique. Metal forming is an economical method of manufacturing components because loss of material is too less. It is a process in which the desired shapes and size of components are obtained through the plastic deformation of metal. Sheet metals are widely used for industrial and consumer parts because of its capacity for being bent and formed into intricate shapes. Sheet metal parts comprise a large fraction of automotive, agricultural machinery, and aircraft components as well as consumer appliances. II. FORMING PARAMETERS Successful sheet metal forming operation depends on the selection of punch nose radius, die arc radius, punch velocity, blank holding force, spring back, blank size and shape, die clearance and lubrication. Forming limit diagram (FLD) and circle grid analysis helps to understand forming in sheet metals. The summary of some of the works conducted by different researchers regarding forming is listed below; they described the analytical approach and experimental results. 2.1 Punch nose radius Dr.Waleed K.Jawad ,Jamal H.Mohamed[1] studied the effect of punch nose radius on deep drawing operation. In this work, six types of punches with various nose radii have been used to form a cylindrical cup of (44mm) outer diameter,(28mm) height, and(0.5mm)sheet thickness of mild steel of (0.15%) carbon content. A commercially finite element program code (ANSYS 5.4), was used to perform the numerical simulation of the deep drawing operation, and the numerical results were compared with the experimental work. The results show that, the value of work required to form parts with large www.ijera.com nose radii is much more than the value required to form parts with small punch nose radii. The greatest thinning is seen to occur with hemispherical punch (Dome shaped punch) due to great stretching of the metal over the punch head. The maximum tensile stresses and the maximum thinning of the dome wall occur nearly at the apex of the dome. 2.2 Blank temperature G. Venkateswarlu, M. J. Davidson and G. R. N. Tagore[2] extensively studied formability aspects of aluminium 7075 to develop useful components of complex shapes. In that study, the significance of three important deep drawing process parameters namely blank temperature, die arc radius and punch velocity on the deep drawing characteristics of aluminium 7075 sheet was determined. The combination of finite element method and Taguchi analysis was used to determine the influence of process parameters. Simulations were carried out as per orthogonal array using DEFORM 2Dsoftware. Based on the predicted deformation of deep drawn cup and analysis of variance test (Anova), it was observed that blank temperature has greatest influence on the formability of aluminium material followed by punch velocity and die arc radius. 2.3 Blank holding force Y. Marumo, H. Saiki, L Ruan [3] has carried out the study regarding variation in the blank holding force required for the elimination of wrinkling and the limiting drawing ratio with sheet thickness. They found that blank holding force required for the elimination of wrinkling increased rapidly as the sheet thickness decreased. When the sheet thickness was very thin, the blank holding force was strongly influenced by the coefficient of friction. The limiting drawing ratio decreased as sheet thickness decreased and it decreased rapidly below 0.04 mm thickness. 300 | P a g e
  • 2. U. V. Mangudkar et al Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303 When the sheet thickness was very thin, the limiting drawing ratio was strongly influenced by the coefficient of friction. 2.4 Intital blank shape M. Ahmetoglu, T. R. Broek, G. Kinzel, T. Altan [4] have carried out the study of effect of process parameters such as initial blank shape and the blank holding force on the final part quality (i.e., wrinkling and fracture). During the initial experiments, it was found that the oval blank shape had the worst formability, from a fracture point of view, among the three blank shapes (i.e., oval, oblong, and rectangle). The oval shape reduced the fracture limit of AA 2008-T4. However, it caused smaller wrinkling heights in the flange along the sides of the rectangular pan. Control of the (BHF) as a function of time improves the formability and the quality of the final part. However, BHF control in time is not enough by itself. Since the deformation characteristics are not uniform around the periphery of the rectangle, the BHF has to be controlled as a function of location, too. Metal flow can be controlled by using draw beads on the sides of the rectangle. 2.5 An optimization strategy for the blank holder force (BHF) H. Gharib, A.S. Wifi, M. Younan, A. Nassef [5] have proposed an optimization strategy for the blank holder force (BHF) which searches for the BHF scheme that minimizes the maximum punch force and avoids process limits. That strategy was applied to the linearly varying BHF scheme and compared to the constant BHF. They found that the optimized linear BHF scheme resulted in an improved cup forming when compared to that produced by the constant BHF scheme. The BHF scheme is optimized for different cases of drawing ratios and die coefficients of friction in order to analyze the nature of the optimum linear BHF scheme. It was found that the slope of the linear BHF scheme increases with the increase in the drawing ratio in a linear manner. Also, the intercept of the function showed a nearly linear variation with the drawing ratio. A general equation is deduced for the optimum blank holder force at any drawing ratio for the cup under study. 2.6 Spring back W.M. Chan, H.I. Chew, H.P. Lee, B.T. Cheok [6] have presented a study of spring-back in the V-bending metal forming process with one clamped end and one free end. They found that spring-back occurs at the die-lip and V-region of the die model. Different die punch parameters such as punch radius, punch angle and die-lip radius were varied to study their effect on spring-back. Also, the effect of the punch displacement on spring-back was investigated. The H-convergence test was done to justify the number of elements used. Softwares used are Patran, Abaqus/Standard and Abaqus/CAE. Patran www.ijera.com www.ijera.com was used to model the nodes of the sheet metal and rigid surfaces of the die, pad and punch. Abaqus/Standard is used to simulate the punching process. The results were analyzed using Abaqus/CAE. Their analysis shows that spring-back angle of the valley region decreased with increment of punch radius and punch angle and spring-back is dependent on punch radius, punch angle and die-lip radius. III. FORMING LIMIT DIAGRAM The forming limit diagram (FLD) (Fig.3.1) gives an indication whether the material can sustain certain ratio of strains without failing is of great help. Keeler[7] pioneered the application of forming limit diagrams (FLD) for accessing the formability of sheet metal. Fig.3.1 Forming limit diagram[8] Many researchers have tried to determine the FLD diagrams for different sheet metals commonly used in forming operations either experimentally or theoretically. The experimental method consists of printing a grid pattern of circles of appropriate diameter (generally 2 mm to 4 mm) on the surface of sheet. The sheet is deformed as required but in stages. After each stage the grid pattern is examined. The advantage of printing circular grids is that during the deformation the circles will get deformed into ellipse with major and minor axes directed along the principal directions of strain. The measurement of the axes and knowing the original diameter we can determine principal strains and their directions. As the forming progresses, at some region neck formation may occur. The ratio of strains is determined at the region. This is a point on FLD diagram or curve which separates the safe and unsafe regions. In 1967, Marciniak and Kuczynski proposed their analytical model for limit-strain prediction based on the initial in homogeneity of a material, which has been foundational for much of the subsequent work in this area and is commonly referred to as theM–K theory [9]. They attributed changes in limiting strain values to the loading history of the specimen, the ratio of the principal stresses, and several material 301 | P a g e
  • 3. U. V. Mangudkar et al Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303 properties, including the initial in homogeneity. They noted that the largest limiting strains in the biaxial stretching region were obtained during equal biaxial tension, whilst the minimum values occurred in plane-strain.One of the primary applications of the circular grid system and FLD proposed by Keeler was the analysis of strain distributions in actual stampings to improve part quality and optimize die design [10]. Since Keeler’s experiments continued to verify his earlier results, showing that the lowest formability exists under plane strain conditions, he proposed restricting the inward flow of metal from the flange in order to induce biaxial tensile strains, thereby increasing the forming limits. The preceding studies focused on the determination of forming limits solely in the region of biaxial tension. However, in 1968, Goodwin used a combination ofcup- and tension-tests to obtain a failure band in both the negative and positive quadrants of minor strain, creating the general form of the forming-limit diagram. In order to reveal the effects of planar anisotropy on formability, Marciniak et al. performed an experimental study involving steel, aluminum, and copper [11]. These tests were performed under proportional-straining conditions, and showed that the forming limits were significantly different in the rolling direction compared with transverse direction. This demonstrated that the limit curve does not consist of mirror images which begin at the principal axes and meet at the state of equal biaxial tension; instead, the limit strains are generally somewhat greater in the rolling direction. A further investigation of variations in the forming limit diagram was conducted by Ghosh and Hecker, who concluded that the limit strains obtained in punch stretching operations were considerably higher than those resulting from in-plane stretching tests [12,13]. Their in-plane stretching tests employed the use of a polyethylene spacer on either side of the nose of a punch in order to induce in-plane deformation. They theorized that the friction and curvature present during punch stretching cause strain localization to take place at a much lower rate than for in-plane stretching. Up to this point, most work on constructing the forming-limit diagram had employed the use of grid strain analysis on actual automotive stampings or on test specimens deformed by punches of various geometries. In 1975, Hecker introduced a methodical approach involving the stretching of sheets of various widths over a hemispherical punch to obtain strain conditions ranging from uniaxial tension to balanced biaxial tension[14]. Using the onset of localized necking to define a single limit of failure, Hecker obtained a forming-limit curve lying mostly within the Keeler– Goodwin band. The advantage of his technique is the ability to determine an entire forming-limit curve with specimens of different widths and:or the use of different lubricants. An analytical model describing neck growth in sheet metals under various loading conditions, from which www.ijera.com www.ijera.com a predicted forming-limit diagram can be calculated, was subsequently developed by Lee and Zaverl [15]. Their results corresponded to those of the lower, inplane forming limits. However, the analysis did not account for the effects of strain history and its influence on such properties as the plastic strain ratio. IV. SUMMARY The forming limit diagram (FLD) introduced by Keller and Goodwin probably the most widely used method for representing sheet metal formability and extensive literature has been proposed in the last decade. The forming limit diagram typically represents the maximum permissible range of major and minor strains that a typical sheet material can undertake without failure. The forming limit diagram is experimentally measured for each sheet material by placing a grid of circle on the sheet sample and then deforming the same. A comparison of the original and the extensions in the marked grids on the sheet sample provide an estimate of the major and minor strain of the sample. The permissible range of the major and minor strains is actually available for a wide range of sheet metals and used considerably for designing of deep drawing operations, in particular. REFERENCES [1] Dr.Waleed K.Jawad,Jamal H.Mohamed, “Studying the Effect of Punch Nose Radius on Deep Drawing Operation” Eng.&Tech.Vol.26.No.,pp55-73(2008) [2] G. Venkateswarlu, M. J. Davidson and G. R. N. Tagore, “Influence of process parameters on the cup drawing of aluminium 7075 sheet” International Journal of Engineering, Science and Technology Vol. 2, No. 11, pp. 41-49(2010) [3] Y. Marumo, H. Saiki, L Ruan , “Effect of sheet thickness on deep drawing of metal foils” Journal of Achievements in Materials and Manufacturing Engineering Vol.20 Issues 1-2 (2007) [4] M. Ahmetoglu, T. R. Broek, G. Kinzel, T. Altan, “Control of Blank Holder Force to Eliminate Wrinkling and Fracture in DeepDrawing Rectangular Parts” Annals of the ClRP Vol. 44/1/1995 [5] H. Gharib, A.S. Wifi, M. Younan, A. Nassef, “Optimization of the blank holder force in cup drawing ” Journal of Achievements in Materials and Manufacturing Engineering, Volume 18, ISSUE 1-2 September–October 2006 [6] W.M. Chan, H.I. Chew, H.P. Lee, B.T. Cheok , “Finite element analysis of springback of V-bending sheet metal forming processes” Journal of Materials Processing Technology Vol.148 pp 15–24, (2004) [7] Keeler, S.P.; Sheet Met.Indust.,Vol.42. pp.683,1965 302 | P a g e
  • 4. U. V. Mangudkar et al Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 6, Nov-Dec 2013, pp.300-303 [9] [10] [11] [12] [13] [14] [15] www.ijera.com Z. Marciniak, K. Kuczynski, “ Limit strains in the process of stretch-forming sheet metal” Int. J. Mech. Sci. 9 (1967) 609–620. S.P. Keeler, “Circular grid system—A valuable aid for evaluatingsheet metal formability” Society of Automotive Engineers Technical Paper No. 680092, New York, 1968. Z. Marciniak, K. Kuczynski, T. Pokora, “ Influence of the plastic properties of a material on the forming limit diagram for sheet metal in tension” Int. J. Mech. Sci. 15,pp 789–805,1973. A.K. Ghosh, S.S. Hecker, “Stretching limits in sheet metals:In-plane versus out-of-plane deformation” Metall. Trans. 5,pp 2161– 2164,(1974) S.S. Hecker, “Experimental studies of sheet stretchability,Formability: Analysis, Modeling and Experimentation”, Proceedings October 1977 AIME:ASM Symposium, “The Metallurgical Society of the American Institute of Mining, Metallurgical and Petroleum Engineers” pp. 150–182 New York, 1978,. S.S. Hecker, “Simple technique for determining forming limit curves”, Sheet Met. Ind. 52, pp671–676 (1975). D. Lee, F. Zaverl Jr., “ Neck growth and forming limits in sheet metals”, Int. J. Mech. Sci. 24 (3) pp.157–173(1982). Books: [8] Kalpakjain, Manufacturing Processes for Engineering Materials ( Pearson Education, 2007 ) www.ijera.com 303 | P a g e