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P. Pratihar Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016

RESEARCH ARTICLE

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OPEN ACCESS

Dynamic Drape Behavior of Textile Fabric: Part I - Development
of an Instrument and Its Implications
P. Pratihar
Department of Textile Engineering Faculty of Technology and Engineering, The Maharaja Sayajirao University
of Baroda, Vadodara, Gujarat, India

Abstract
There are instruments available to measure the drape coefficient of fabric. The most widely accepted method (IS
8357:1977) is hang a circular fabric sample and measure the drape coefficient. This measurement technique
gives quite a bit of fair idea about drape coefficient of a fabric in static condition. But when it’s static condition
is disturbed as the case in practical application of fabric in the form of using as garment or in the form of any
domestic application like using it as curtain or table cloth, it’s shape of fabric fall pattern i.e nodes in term of
drape terminology changes. Therefore, to get some idea about the effect of above mentioned static condition to
dynamic condition of the fabric, a need was felt to have some sort of simulation. Here simulation might not be
possible exactly to the practical condition, but one can think of some sort of simulation, similar to it and find out
the effect of the same on drape properties of fabric. Therefore, it was thought that some simple, inexpensive,
easy to handle instrument would be developed to measure the dynamic drape coefficient of fabric. The present
work is the result of the same.
Keyword:- drape, drape coefficient, instrument, dynamic drape, simulation
I.
INTRODUCTION
The ancient Greeks successfully modeled
fabric drape as a static geometrical system in their
stone statues. They started a mathematics of movement
in which curves were thought of as tracings made by
moving points. Curves were also analyzed instant by
instant trough the technique of slicing into infinitely
fine segments. The first study in deformations of
fabrics was conducted by Peirce (Peirce, 1937) [1].
There are subjective and objective methods to
evaluate drape. The method of objective measurement
of drape is basically fabric fall by itself in specific
shape according to its properties, when part of it is
supported and rest is unsupported. Studies of drape
were first begun by C. C. Chu, when he published a
measuring method for fabric drape using FRL drape
meter(1950) [2]. The measurement of drape, factors
affecting drape and its use has been further discussed
by Chu et al. (1960) [3] and Cusick (1961, 1965, 1968)
[4,5,6]. The most widely accepted method of drape
test is IS 8357:1977
For many decades, much of the textile
literature has been devoted to find linear relation to
explain the natural way in which fabrics deform or
drape. However, linear concept is not applied for
essentially nonlinear phenomena which occur in the
dynamic interactive processes involved in textile and
apparel manufacture and technology (Postle 1995)
[7,8].
The
mechanical
analysis
of
fabric
deformation is expanding the application of computer
simulation and computer aided design. In last couple of
decades many researchers have given due
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concentration in the area of 3D deformation of fabric,
dynamic condition of fabric, simulation and modeling
of fabric drape etc. Some of them to mention here are
particle-based model for simulating the draping of
woven cloth by Breen et al. [9], physical based model
of fabric drape using flexible shell theory by Chen et
al. [10], modelling the dynamic drape of garments by
Stylios et al. [11], drape simulation of woven fabrics
by using explicit dynamic analysis by Yu et al. [12],
modeling a fabric drape profile by Lo et al. [13].
The testing device is designed by Yang et al.
[14] and they defined dynamic drapeability. They has
explained many parameters of dynamic condition of
fabric like effect revolution of fabric, effect of airflow
etc. Dynamic drape study seems to be useful as opined
by Matsudaira & Yang [15], from their work on silk
fabrics for categorizing the fabric.
Therefore, it is obvious that dynamic drape
behavior and dynamic drape coefficient are gaining
more and more popularity day by day. It is so, because
it gives to some extent close to real life situation. Many
research workers in abroad are working on the same
since last decade, but unfortunately very few
information, particularly no data base information is
available. No readymade instrument is available here
to study the dynamic drape behaviour of fabric.
In the present work the main emphasis has
been given to develop an instrument that will be very
simple, easy to use and inexpensive. Accordingly an
instrument has been developed keeping above
mentioned point in mind and it is described in the
following section.

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P. Pratihar Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016
II.

FABRICATION OF THE
INSTRUMENT

A. Fabrication of the Instrument
For the fabrication of the instrument, detailed
drawings has been made by using Auto-CAD based on
the literature studied and in consultation with various
experts in the relevant field. The instrument has been
fabricated with the help of M/s A. J. Engineers,
G.I.D.C., Makarpura, Baroda, Gujarat, India.
The stages of development of the Dynamic
drape tester is not much relevant here, but it will be
highly unjustified if some information regarding it is
not provided here, because it will help others who will
read this report, to understand some of the technical
procedural aspect which need to take care since
beginning of any development and it may help to save
cost as well as time.
In the process of the fabrication of the
instrument, some of the major technical problems
which were encountered, and to solve those issues
various alternatives were tried and the final outcome of
the same are described below with a brief outlines of
the problems encountered and the way it was solved
and the final instrument is developed.
The first important issue was to decide upon
the location of the motor. Initially it was thought of
that the motor would be mounted at the base of the
instrument i.e. inside the base rectangular box. It was
decided so, because, if the motor is mounted at the
upper part of the instrument, there will be problem of
vibration. But, due to insufficient space and some more
other technical problems like, transmitting the drive
and the reduction of the speed, etc. it was not possible
to put it there. So, it was decided to place it at the side
stand of the instrument. To avoid vibration, it was
thought to place the motor at the bottom part of the
side stand. But, unfortunately it was also not possible
to do so, because the supporting stand of the disk
holder was obstructing the free fall of the fabric and it

Fig. 1: Assembly drawings of dynamic drape tester

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could not be managed by placing the motor in this
position. Therefore, finally the motor had to place
towards the upper side of the side stand only.
The next most important problems were to
bring down the speed of the testing disk to minimum
level to about 20-30 rpm. which is required. As per the
requirement, one single phase A.C. motors need to be
attached to the system to give drive. Generally, the
single-phase motor of small size and with low rpm is
not available in the local market. The minimum rpm of
the motor that could be managed from local market
was 1440, but the motor need to run with low rpm by
potentiometer. The motor was not taking load beyond a
certain minimum r.p.m. and this was about 350-400
rpm. Therefore, even after putting motor pulley and the
disk pulley ratio as 1:5, the minimum rpm of the disk
that was possible to achieve was about 80 rpm.
Therefore, it was thought that the problem will be
shorted out by modifying transmission of the drive. In
consultation with various experts and a thorough
brainstorming, various alternatives were thought of and
tried couple of ideas, but initially failed.
Finally, one small converter gearbox was
managed from Ahmedabad, Gujarat, India which
helped to solve the problem partially. Partially in the
sense, when the speed is brought down and achieved
about 20rpm of the sample holder disk, but the next
problem was the higher side of the rpm. With this
attachment maximum rpm that was possible was about
80. Therefore, again the drive had to be modified and
made a two steps pulley. With the second step of the
pulley, the maximum rpm of the sample holder disk
that could achieve is about 180 r.p.m, which is good
enough for our existing purpose. Therefore, this was
accepted and the assembly was fixed up. Some of the
important drawings of the assembly of the instrument
are given in Fig 1 to 3 and photograph of the
instrument is given in the Fig. 4.

Fig. 2: Assembly drawings of dynamic drape tester

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P. Pratihar Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016

Fig. 3: Assembly drawings of dynamic drape tester
The instrument has some special feature
attached to it. One of its unique feature is automatic
time settings. Time for rotational motion of the disk
could be set and after the preset time is elapsed, the
motor will automatically stops. The time could be set
from 9.99 seconds to 999 hours. Therefore, a wide
range of settings can be done and experimental plan
can be set accordingly.
The instrument has auto standby mode on
each segment. It means on power cut or on-off of
main switch, it will go to standby mode, which will
Sample
No.
S1
S2

Count (Ne)
Warp
Weft

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Fig. 4: Photograph of the Fabricated Instrument
save the instrument from any undue damage due to
power cuts. Digital Display of r.p.m . of the disk
already mentioned earlier. Because of the same it is
possible to set the experimentation parameters very
precisely.
B. Illustrative Study of Dynamic Drape Behaviour
To illustrate the study of dynamic drape
behaviour of the fabric of the above mentioned
instrument, two suiting fabric samples – a plain and a
twill(2/1) of following particulars have been taken:
Yarn Density
EPI
PPI

Weave

14

14

56

52

Plain

13

16

76

56

2/1 Twill

These fabric Samples were measured for
for almost all the cases there is increase in drape
drape coefficient at the five levels of rotations
coefficient with the increase in r.p.m. It can also be
(clockwise) i.e. 0, 25, 75, 125 & 175. The test data
noticed that compare to static (initial drape
are given in the following table no. 1& 2, Graphical
coefficient without revolutions), the change in drape
representations of these data are shown in chart no. 1
coefficient with 25 r.p.m. in almost all the cases as
to 4. In the charts, the series (i), represent drape
well as for some cases with 75 r.p.m. also, is not
coefficient at different r.p.m. and the series (ii)
much. In case of higher r.p.m. i.e. 125 and more there
represent number of nodes at different r.p.m. The
is increase in drape coefficient. It can also be noticed
series (a) represent the trend line drawn by using
from the charts of number of nodes and the series (ii)
linear equations and the series (b) by using
that increase in drape coefficient is highly associated
logarithmic scale.
with number of nodes. As the number of nodes
From the above mentioned tables i.e.1 & 2
increases, the drape coefficient also increases.
and the charts i.e. 1 to 4, in general it can be seen that
Table No. 1: Sample No. S1: Drape Coefficient at Different rpm (clockwise rotation)
Face
Back
RPM Draped
Drape
Draped
Drape
Area
coefficient% Nodes
Area
coefficient% Nodes
0
281
43.0
5
276
41.6
4
25
284
43.8
5
276
41.6
4
75
286
44.4
5
290
45.4
5
125
293
46.3
6
300
48.2
7
175
297
47.3
7
306
49.8
8

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1014 | P a g e
Drape Co-efficient %

P. Pratihar Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016

www.ijera.com

Chart No. 1: Drape Co-efficient of Sample No. S1 at different rpm, rotating
clockwise
y = 2.2817x + 38.484
50.0
R² = 0.9443
47.5
y = 1.1137x + 41.608
45.0
R² = 0.9617
42.5
40.0

0
43.0
41.6

Front
Back

25
43.8
41.6

75
44.4
45.4

125
46.3
48.2

175
47.3
49.8

Rotational Speed, rpm

No. of Nodes

Chart No. 2: Number of Nodes for Sample no. S1 at different rpm
10
8
6
4
2
0

0
5
4

Front
Back

25
5
4

75
5
5

125
6
7

175
7
8

Rotational Speed, rpm
Table No. 2: Sample No. S2: Drape Coefficient at Different rpm (clockwise rotation)
RPM

Drape Co-efficient %

0
25
75
125
175

Draped
Area
334
338
339
349
351

Chart No.3:

Face
Drape
coefficient%
57.4
58.5
58.7
61.5
62.0

Nodes
5
5
5
5
5

Draped
Area
330
331
341
345
349

Nodes
5
5
5
6
7

Drape Co-efficient of Sample No. S2 at different rpm, rotating clockwise

64.0

y = 1.4125x + 54.565
R² = 0.9494

y = 1.2223x + 55.95
R² = 0.9255

61.0

Back
Drape
coefficient%
56.3
56.6
59.3
60.4
61.5

58.0
55.0
Front
Back

0
57.4
56.3

25
58.5
56.6

75
58.7
59.3

125
61.5
60.4

175
62.0
61.5

Rotational Speed, rpm

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1015 | P a g e
P. Pratihar Int. Journal of Engineering Research and Application
ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016

www.ijera.com

No. of Nodes

Chart No. 4: Number of Nodes for Sample No. S2 at different rpm
8
6
4
2
0

0
5
5

Front
Back

25
5
5

75
5
5

125
5
6

175
5
7

Rotational Speed, rpm

III.

CONCLUSION

An instrument has successfully been
fabricated with various digital display and other
required features for measuring dynamic drapeability
of fabric, which will help in future for various studies
undertaken by the various researchers. The
illustrative study mentioned above indicates, some
trend has been observed in these cases of the fabric
tested. As the rotational rpm of the fabric increased,
it’s drape coefficient also increased. Trend is more
prominent for the fabric samples whose drape
coefficient is low i.e. limpy fabric, as in the case of
fabric sample S1.
The preliminary work carried out here in the
newly fabricated instrument substantiates many of
the work done in the past as mentioned earlier. More
elaborative study is required on the said instrument to
conclude the same with more clarity and evidence.
Apart from that it can be claimed that the instrument
is very simple and facilitate objective measurement
of dynamic drape properties of fabric. Study of
correlation between various mechanical and
processing parameters of the fabric and their
relationship with dynamic drapeability of fabric can
be studied using the said instrument. It should be
very much useful by various stakeholders like fabric
manufacturer, process house, quality control
department, garment manufacturer, researchers, etc.
We are very much hopeful that the instrument will
find its new arena of application.

IV.

ACKNOWLEDGEMENT

I take this opportunity to express my
profound gratitude and deep regards to Professor
Someshwar S Bhattacharya for his exemplary
guidance, monitoring and constant encouragement
throughout the development of the instrument.

[3].

[4].
[5].
[6].
[7].
[8].

[9].

[10].

[11].

[12].

[13].

[14].

REREFENCES
[1].

[2].

Peirce, F.T., (1937) The geometry of cloth
structure. Journal of the Textile Institute, Vol.28,
No. T45, pp.43-77.
Chu C C, Cumings C L and Teixeira N A (1950),
“Mechanics of Elastic Performance of Textile
Materials, Part V: A Study of the Factors
Affecting the Drape of Fabrics – The

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[15].

Development of a Drape Meter”, Text. Res. J.,
20(8), pp 539-548.
Investigation of the Factors Affecting the
Drapeability of Fabrics by C. C. Chu, M. M. Platt
and W. J. Hamburger Text. Res. J., 30, 66-67
(1960).
The resistance of fabric to shear forces by G. E.
Cusick, J. Text. Inst., 52(9), T395-T406 (1961).
The measurement of fabric drape by G. E.
Cusick, J. Text. Inst., 59(6), T253-T260 (1965).
The measurement of Fabric Drape J. Text. Inst.,
vol 59, pp. 253-260
Fabric Drape by Jacqueline R. Postle and Ron
Postle, Textile Asia, Jan. 2000, pp 30-32.
Modelling fabric deformation as a non-linear
dynamical
system
using
Backlund
transformations, Special Edition of International
Journal of Clothing Science and Technology, vol
8, No. 3.
A Particle-Based Model for Simulating the
Draping Behaviour of Woven Cloth by David E.
Breen, Donald H. House and Michal J. Wozny,
Text. Res. J., 64(11), 663-685(1994).
A Physical Based Model of Fabric Drape Using
Flexible Shell Theory by B. Chen and M.
Govindaraj, Text. Res. J., 65, 324-330 (1995).
Modelling the dynamic drape of garments on
synthetic humans in a virtual fashion show by
George K. Stylios, T. R. Wan and N. J. Powell,
International Journal of Clothing Science and
Technology, vol 8, No. 3, 1996, pp. 95-112.
Drape Simulation of Woven Fabrics by Using
Explicit Dynamic Analysis by W. R. Yu. T. J.
Kang and K. Chung, J. Text. Inst., 2000, vol 91,
part 1, No. 2 pp. 285-301.
Modeling a fabric drape profile by W. M. Lo, J.
L. Hu and L. K. Li, Text. Res J., 2003, 72(5), pp.
454-463 (2002).
Measurement of drape coefficients of fabrics and
description of hanging shapes of fabrics Part 4:
Evaluation and dynamic drape behavior of fabrics
using a testing device by Yang M. and
Matsudaira M., Journal of the Textile Machinery
Society of Japan, 1999; 52(9), T167-T175(1999).
Features of conventional static and new dynamic
drape coefficients of woven silk fabrics by
Matsudaira M. & Yang M., Text. Res J., 2003,
73(3), pp. 250-255.

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  • 1. P. Pratihar Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016 RESEARCH ARTICLE www.ijera.com OPEN ACCESS Dynamic Drape Behavior of Textile Fabric: Part I - Development of an Instrument and Its Implications P. Pratihar Department of Textile Engineering Faculty of Technology and Engineering, The Maharaja Sayajirao University of Baroda, Vadodara, Gujarat, India Abstract There are instruments available to measure the drape coefficient of fabric. The most widely accepted method (IS 8357:1977) is hang a circular fabric sample and measure the drape coefficient. This measurement technique gives quite a bit of fair idea about drape coefficient of a fabric in static condition. But when it’s static condition is disturbed as the case in practical application of fabric in the form of using as garment or in the form of any domestic application like using it as curtain or table cloth, it’s shape of fabric fall pattern i.e nodes in term of drape terminology changes. Therefore, to get some idea about the effect of above mentioned static condition to dynamic condition of the fabric, a need was felt to have some sort of simulation. Here simulation might not be possible exactly to the practical condition, but one can think of some sort of simulation, similar to it and find out the effect of the same on drape properties of fabric. Therefore, it was thought that some simple, inexpensive, easy to handle instrument would be developed to measure the dynamic drape coefficient of fabric. The present work is the result of the same. Keyword:- drape, drape coefficient, instrument, dynamic drape, simulation I. INTRODUCTION The ancient Greeks successfully modeled fabric drape as a static geometrical system in their stone statues. They started a mathematics of movement in which curves were thought of as tracings made by moving points. Curves were also analyzed instant by instant trough the technique of slicing into infinitely fine segments. The first study in deformations of fabrics was conducted by Peirce (Peirce, 1937) [1]. There are subjective and objective methods to evaluate drape. The method of objective measurement of drape is basically fabric fall by itself in specific shape according to its properties, when part of it is supported and rest is unsupported. Studies of drape were first begun by C. C. Chu, when he published a measuring method for fabric drape using FRL drape meter(1950) [2]. The measurement of drape, factors affecting drape and its use has been further discussed by Chu et al. (1960) [3] and Cusick (1961, 1965, 1968) [4,5,6]. The most widely accepted method of drape test is IS 8357:1977 For many decades, much of the textile literature has been devoted to find linear relation to explain the natural way in which fabrics deform or drape. However, linear concept is not applied for essentially nonlinear phenomena which occur in the dynamic interactive processes involved in textile and apparel manufacture and technology (Postle 1995) [7,8]. The mechanical analysis of fabric deformation is expanding the application of computer simulation and computer aided design. In last couple of decades many researchers have given due www.ijera.com concentration in the area of 3D deformation of fabric, dynamic condition of fabric, simulation and modeling of fabric drape etc. Some of them to mention here are particle-based model for simulating the draping of woven cloth by Breen et al. [9], physical based model of fabric drape using flexible shell theory by Chen et al. [10], modelling the dynamic drape of garments by Stylios et al. [11], drape simulation of woven fabrics by using explicit dynamic analysis by Yu et al. [12], modeling a fabric drape profile by Lo et al. [13]. The testing device is designed by Yang et al. [14] and they defined dynamic drapeability. They has explained many parameters of dynamic condition of fabric like effect revolution of fabric, effect of airflow etc. Dynamic drape study seems to be useful as opined by Matsudaira & Yang [15], from their work on silk fabrics for categorizing the fabric. Therefore, it is obvious that dynamic drape behavior and dynamic drape coefficient are gaining more and more popularity day by day. It is so, because it gives to some extent close to real life situation. Many research workers in abroad are working on the same since last decade, but unfortunately very few information, particularly no data base information is available. No readymade instrument is available here to study the dynamic drape behaviour of fabric. In the present work the main emphasis has been given to develop an instrument that will be very simple, easy to use and inexpensive. Accordingly an instrument has been developed keeping above mentioned point in mind and it is described in the following section. 1012 | P a g e
  • 2. P. Pratihar Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016 II. FABRICATION OF THE INSTRUMENT A. Fabrication of the Instrument For the fabrication of the instrument, detailed drawings has been made by using Auto-CAD based on the literature studied and in consultation with various experts in the relevant field. The instrument has been fabricated with the help of M/s A. J. Engineers, G.I.D.C., Makarpura, Baroda, Gujarat, India. The stages of development of the Dynamic drape tester is not much relevant here, but it will be highly unjustified if some information regarding it is not provided here, because it will help others who will read this report, to understand some of the technical procedural aspect which need to take care since beginning of any development and it may help to save cost as well as time. In the process of the fabrication of the instrument, some of the major technical problems which were encountered, and to solve those issues various alternatives were tried and the final outcome of the same are described below with a brief outlines of the problems encountered and the way it was solved and the final instrument is developed. The first important issue was to decide upon the location of the motor. Initially it was thought of that the motor would be mounted at the base of the instrument i.e. inside the base rectangular box. It was decided so, because, if the motor is mounted at the upper part of the instrument, there will be problem of vibration. But, due to insufficient space and some more other technical problems like, transmitting the drive and the reduction of the speed, etc. it was not possible to put it there. So, it was decided to place it at the side stand of the instrument. To avoid vibration, it was thought to place the motor at the bottom part of the side stand. But, unfortunately it was also not possible to do so, because the supporting stand of the disk holder was obstructing the free fall of the fabric and it Fig. 1: Assembly drawings of dynamic drape tester www.ijera.com www.ijera.com could not be managed by placing the motor in this position. Therefore, finally the motor had to place towards the upper side of the side stand only. The next most important problems were to bring down the speed of the testing disk to minimum level to about 20-30 rpm. which is required. As per the requirement, one single phase A.C. motors need to be attached to the system to give drive. Generally, the single-phase motor of small size and with low rpm is not available in the local market. The minimum rpm of the motor that could be managed from local market was 1440, but the motor need to run with low rpm by potentiometer. The motor was not taking load beyond a certain minimum r.p.m. and this was about 350-400 rpm. Therefore, even after putting motor pulley and the disk pulley ratio as 1:5, the minimum rpm of the disk that was possible to achieve was about 80 rpm. Therefore, it was thought that the problem will be shorted out by modifying transmission of the drive. In consultation with various experts and a thorough brainstorming, various alternatives were thought of and tried couple of ideas, but initially failed. Finally, one small converter gearbox was managed from Ahmedabad, Gujarat, India which helped to solve the problem partially. Partially in the sense, when the speed is brought down and achieved about 20rpm of the sample holder disk, but the next problem was the higher side of the rpm. With this attachment maximum rpm that was possible was about 80. Therefore, again the drive had to be modified and made a two steps pulley. With the second step of the pulley, the maximum rpm of the sample holder disk that could achieve is about 180 r.p.m, which is good enough for our existing purpose. Therefore, this was accepted and the assembly was fixed up. Some of the important drawings of the assembly of the instrument are given in Fig 1 to 3 and photograph of the instrument is given in the Fig. 4. Fig. 2: Assembly drawings of dynamic drape tester 1013 | P a g e
  • 3. P. Pratihar Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016 Fig. 3: Assembly drawings of dynamic drape tester The instrument has some special feature attached to it. One of its unique feature is automatic time settings. Time for rotational motion of the disk could be set and after the preset time is elapsed, the motor will automatically stops. The time could be set from 9.99 seconds to 999 hours. Therefore, a wide range of settings can be done and experimental plan can be set accordingly. The instrument has auto standby mode on each segment. It means on power cut or on-off of main switch, it will go to standby mode, which will Sample No. S1 S2 Count (Ne) Warp Weft www.ijera.com Fig. 4: Photograph of the Fabricated Instrument save the instrument from any undue damage due to power cuts. Digital Display of r.p.m . of the disk already mentioned earlier. Because of the same it is possible to set the experimentation parameters very precisely. B. Illustrative Study of Dynamic Drape Behaviour To illustrate the study of dynamic drape behaviour of the fabric of the above mentioned instrument, two suiting fabric samples – a plain and a twill(2/1) of following particulars have been taken: Yarn Density EPI PPI Weave 14 14 56 52 Plain 13 16 76 56 2/1 Twill These fabric Samples were measured for for almost all the cases there is increase in drape drape coefficient at the five levels of rotations coefficient with the increase in r.p.m. It can also be (clockwise) i.e. 0, 25, 75, 125 & 175. The test data noticed that compare to static (initial drape are given in the following table no. 1& 2, Graphical coefficient without revolutions), the change in drape representations of these data are shown in chart no. 1 coefficient with 25 r.p.m. in almost all the cases as to 4. In the charts, the series (i), represent drape well as for some cases with 75 r.p.m. also, is not coefficient at different r.p.m. and the series (ii) much. In case of higher r.p.m. i.e. 125 and more there represent number of nodes at different r.p.m. The is increase in drape coefficient. It can also be noticed series (a) represent the trend line drawn by using from the charts of number of nodes and the series (ii) linear equations and the series (b) by using that increase in drape coefficient is highly associated logarithmic scale. with number of nodes. As the number of nodes From the above mentioned tables i.e.1 & 2 increases, the drape coefficient also increases. and the charts i.e. 1 to 4, in general it can be seen that Table No. 1: Sample No. S1: Drape Coefficient at Different rpm (clockwise rotation) Face Back RPM Draped Drape Draped Drape Area coefficient% Nodes Area coefficient% Nodes 0 281 43.0 5 276 41.6 4 25 284 43.8 5 276 41.6 4 75 286 44.4 5 290 45.4 5 125 293 46.3 6 300 48.2 7 175 297 47.3 7 306 49.8 8 www.ijera.com 1014 | P a g e
  • 4. Drape Co-efficient % P. Pratihar Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016 www.ijera.com Chart No. 1: Drape Co-efficient of Sample No. S1 at different rpm, rotating clockwise y = 2.2817x + 38.484 50.0 R² = 0.9443 47.5 y = 1.1137x + 41.608 45.0 R² = 0.9617 42.5 40.0 0 43.0 41.6 Front Back 25 43.8 41.6 75 44.4 45.4 125 46.3 48.2 175 47.3 49.8 Rotational Speed, rpm No. of Nodes Chart No. 2: Number of Nodes for Sample no. S1 at different rpm 10 8 6 4 2 0 0 5 4 Front Back 25 5 4 75 5 5 125 6 7 175 7 8 Rotational Speed, rpm Table No. 2: Sample No. S2: Drape Coefficient at Different rpm (clockwise rotation) RPM Drape Co-efficient % 0 25 75 125 175 Draped Area 334 338 339 349 351 Chart No.3: Face Drape coefficient% 57.4 58.5 58.7 61.5 62.0 Nodes 5 5 5 5 5 Draped Area 330 331 341 345 349 Nodes 5 5 5 6 7 Drape Co-efficient of Sample No. S2 at different rpm, rotating clockwise 64.0 y = 1.4125x + 54.565 R² = 0.9494 y = 1.2223x + 55.95 R² = 0.9255 61.0 Back Drape coefficient% 56.3 56.6 59.3 60.4 61.5 58.0 55.0 Front Back 0 57.4 56.3 25 58.5 56.6 75 58.7 59.3 125 61.5 60.4 175 62.0 61.5 Rotational Speed, rpm www.ijera.com 1015 | P a g e
  • 5. P. Pratihar Int. Journal of Engineering Research and Application ISSN : 2248-9622, Vol. 3, Issue 5, Sep-Oct 2013, pp.1012-1016 www.ijera.com No. of Nodes Chart No. 4: Number of Nodes for Sample No. S2 at different rpm 8 6 4 2 0 0 5 5 Front Back 25 5 5 75 5 5 125 5 6 175 5 7 Rotational Speed, rpm III. CONCLUSION An instrument has successfully been fabricated with various digital display and other required features for measuring dynamic drapeability of fabric, which will help in future for various studies undertaken by the various researchers. The illustrative study mentioned above indicates, some trend has been observed in these cases of the fabric tested. As the rotational rpm of the fabric increased, it’s drape coefficient also increased. Trend is more prominent for the fabric samples whose drape coefficient is low i.e. limpy fabric, as in the case of fabric sample S1. The preliminary work carried out here in the newly fabricated instrument substantiates many of the work done in the past as mentioned earlier. More elaborative study is required on the said instrument to conclude the same with more clarity and evidence. Apart from that it can be claimed that the instrument is very simple and facilitate objective measurement of dynamic drape properties of fabric. Study of correlation between various mechanical and processing parameters of the fabric and their relationship with dynamic drapeability of fabric can be studied using the said instrument. It should be very much useful by various stakeholders like fabric manufacturer, process house, quality control department, garment manufacturer, researchers, etc. We are very much hopeful that the instrument will find its new arena of application. IV. ACKNOWLEDGEMENT I take this opportunity to express my profound gratitude and deep regards to Professor Someshwar S Bhattacharya for his exemplary guidance, monitoring and constant encouragement throughout the development of the instrument. [3]. [4]. [5]. [6]. [7]. [8]. [9]. [10]. [11]. [12]. [13]. [14]. REREFENCES [1]. [2]. Peirce, F.T., (1937) The geometry of cloth structure. Journal of the Textile Institute, Vol.28, No. T45, pp.43-77. Chu C C, Cumings C L and Teixeira N A (1950), “Mechanics of Elastic Performance of Textile Materials, Part V: A Study of the Factors Affecting the Drape of Fabrics – The www.ijera.com [15]. Development of a Drape Meter”, Text. Res. J., 20(8), pp 539-548. Investigation of the Factors Affecting the Drapeability of Fabrics by C. C. Chu, M. M. Platt and W. J. Hamburger Text. Res. J., 30, 66-67 (1960). The resistance of fabric to shear forces by G. E. Cusick, J. Text. Inst., 52(9), T395-T406 (1961). The measurement of fabric drape by G. E. Cusick, J. Text. Inst., 59(6), T253-T260 (1965). The measurement of Fabric Drape J. Text. Inst., vol 59, pp. 253-260 Fabric Drape by Jacqueline R. Postle and Ron Postle, Textile Asia, Jan. 2000, pp 30-32. Modelling fabric deformation as a non-linear dynamical system using Backlund transformations, Special Edition of International Journal of Clothing Science and Technology, vol 8, No. 3. A Particle-Based Model for Simulating the Draping Behaviour of Woven Cloth by David E. Breen, Donald H. House and Michal J. Wozny, Text. Res. J., 64(11), 663-685(1994). A Physical Based Model of Fabric Drape Using Flexible Shell Theory by B. Chen and M. Govindaraj, Text. Res. J., 65, 324-330 (1995). Modelling the dynamic drape of garments on synthetic humans in a virtual fashion show by George K. Stylios, T. R. Wan and N. J. Powell, International Journal of Clothing Science and Technology, vol 8, No. 3, 1996, pp. 95-112. Drape Simulation of Woven Fabrics by Using Explicit Dynamic Analysis by W. R. Yu. T. J. Kang and K. Chung, J. Text. Inst., 2000, vol 91, part 1, No. 2 pp. 285-301. Modeling a fabric drape profile by W. M. Lo, J. L. Hu and L. K. Li, Text. Res J., 2003, 72(5), pp. 454-463 (2002). Measurement of drape coefficients of fabrics and description of hanging shapes of fabrics Part 4: Evaluation and dynamic drape behavior of fabrics using a testing device by Yang M. and Matsudaira M., Journal of the Textile Machinery Society of Japan, 1999; 52(9), T167-T175(1999). Features of conventional static and new dynamic drape coefficients of woven silk fabrics by Matsudaira M. & Yang M., Text. Res J., 2003, 73(3), pp. 250-255. 1016 | P a g e