1. Field of the Invention
The present invention relates to a method and a device for graphically illustrating the profile for filling a cigarette notably in order to control the strengthening amplitude and the position of strengthened tips relatively to the cut of the stem.
2. Description of the Prior Art
Generally, it is known that cigarette manufacturers have been lead to reduce tobacco density in cigarettes for economical reasons.
The two following questions were then raised:
The retained solution for solving both of these problems was to retain the initial density for the tips (or even strengthen it) and to only reduce the density in the middle of the tobacco section.
It then became necessary to control the strengthening amplitude and the position of the strengthened tips as compared to the cut.
The applicant therefore developed a device for analyzing the filling of cigarettes called ARC, meeting this need.
This device was designed in order to axially displace the cigarettes in a tubular component comprising two diametrically opposite coaxial ports, i.e.:
In this device, a stepper motor drive system causes displacement of the cigarette inside the tubular component. The measuring circuit is then driven in order to record at each step the density of the material crossed by the radiation in the axis of both ports.
This technology was abandoned subsequently because of constraining regulations relating to the handling of radioactive elements.
The applicant then developed another solution consisting of having the cigarette passed through an hyper frequency tuned cavity having a relatively low active thickness, for example of 3 mm. By combining the shift of the tuning frequency and the attenuation of the radiated signal when the cigarette passes through the cavity, it is possible to plot the density profile of the tobacco section of the cigarette.
In one case as in the other, the measured density values are used for obtaining the plot of the density profile of the cigarette.
Nevertheless, the visual interpretation of the plot of the density profile in order to determine with sufficient accuracy the position of the strengthened tips relatively to the cut of the stem and the strengthening amplitude is found to be difficult and uncertain as it depends on the operator.
More particularly, the object of the invention therefore is to determine these parameters automatically.
For this purpose it generally proposes a method based on the observation that the aspect of the density profile of the tobacco section of a cigarette, both with two symmetrical strengthened tips and a single strengthened tip or with two asymmetrical strengthened tips, is periodic and may be modeled as a sinusoidal form.
Considering this observation, the method according to the invention comprises the following operating phases:
Embodiments of the invention will be described hereafter, as non-limiting examples, with reference to the appended drawings wherein:
In the example illustrated in
As an example, the instantaneous density and moisture values will be transferred to the processor 12 by the microcontroller 11 every 50 ms, which corresponds to a 1 mm displacement of the cigarette and to a velocity of 20 mm/s.
Before carrying out a series of measurements, the cigarettes 5 should be sorted into two families illustrated in
After having measured both families, first the filter, the average results of family F2 are reversed (re-establishment of the preparation direction) in order to be processed with family F1.
In the case of cigarettes with two symmetrical strengthened tips BS1, BS2, the density profile is periodical and of a period equal to the length of the tobacco section.
This periodicity appears in
This diagram comprises the plot of a MS1 density sinusoidal model and the curve connecting the measured density MD1 values. A periodic density profile is shown with a period equal to the length of the tobacco section of a cigarette and it fits the following equation:
Y=A0+A1×cos [2×π×(x−φ)/L]
with
With a sinusoidal regression on the measured points (determination coefficient R2), it is possible to automatically determine the strengthening amplitude and the shift of the strengthened tip relatively to the cut C2 (the actual cut C1 is generally shifted relatively to the theoretical cut C2 which is basically located in the middle of a strengthening area corresponding to the stem T).
The determined parameters then are:
It is found that two other types of cigarettes are also proposed on the market, i.e.: cigarettes with a single strengthened tip and cigarettes with two symmetrical strengthened tips.
In the first case, the cigarette comprises a single strengthened tip BD located on the distal end of the cigarette.
In order to determine the density profile and the position of this strengthened tip relatively to the cut, the invention is also based on the observation that this profile is always periodic and that, in this case, the period is equal to double the length of the tobacco section.
This periodicity appears in
Here also, the actual performed cut C1 as well as the theoretical cut C2 are shown in full lines and in dashed lines.
This diagram comprises the plot of a density sinusoidal model MS2 with a period equal to twice the length of the tobacco section of a cigarette and the curve MD2 connecting the measured density values.
The sinusoidal model MS2 used fits the following equation:
y=A0+A1×cos [2×π×(x−φ)/(2×L)]
with
The determined parameters then are:
The position P of the straightened tip is then obtained by the following operating sequence:
If A1<0 then φ=φ+L
P=modulo [φ/(2×L)]
If P<LT−L then P=P+2×L×[int((LT−L−P)/(2×L))+1]
The shift of the strengthened tip BR is obtained by a formula of the type
BR=P−LT
The strengthening index is obtained by a formula of type
IR=2×|A1|
It is found that assembling cigarettes with a strengthened tip BD is delicate because of a certain “softness” of the tobacco section on the filter side.
This is the reason why a conformation of cigarettes, intermediate between the cigarette with two symmetrical strengthened tips as the one illustrated in
Here also, the invention is based on the observation that the density profile is periodic and with a periodicity equal to twice the length of the tobacco.
It proposes to automatically determine the strengthening amplitudes and the shift of the strengthened tip relatively to the cut by means of an even sinusoidal regression of the second order, with a period equal to twice the length of the tobacco.
The sinusoidal model used fits the following equation:
y=A0+A1×cos [2×π×(x−φ)/(2×L)]+A2×cos [4×π×(x−φ)/(2×L)]
with
The determined parameters also are:
The position P of the strengthened tips is obtained by the following operating sequence:
If A1<0 φ=φ+L
the expression of the maximum density value yF of the high-strength tip is
yF=A0+A2−A1
The expression of the maximum density value yf of the low-strength tip is
yf=A0+A1+A2
if A1>0 one has
YF=A0+A1+A2 (maximum density of the high strength tip)
yf=A0+A2−A1 (maximum density of the low strength tip)
The position P of the strengthened tips is obtained by the following operating sequence:
P=modulo [φ/(2×L)]
If P<LT−L then P=P+2×Lx[int((LT−L−P)/(2×L))+1]
The shift of the strengthened tips is obtained by the relationship:
BR=P−LT
Minimum, min=y(x) for x=φ+L/pi×Arccos(−A1/4/A2)
High strengthening index IRF=yF−min
Low strengthening index IRf=yf−min
With the illustrated embodiments in
Nevertheless, the invention is not limited to this solution, it being understood that density measurements may be performed by other techniques such as, for example, the ionization radiation technique (the β ray technique having been set aside exclusively for regulatory matters).
Number | Date | Country | Kind |
---|---|---|---|
04 13168 | Dec 2004 | FR | national |
Number | Name | Date | Kind |
---|---|---|---|
4805641 | Radzio et al. | Feb 1989 | A |
4986285 | Radzio et al. | Jan 1991 | A |
5010904 | Lassiter | Apr 1991 | A |
5347853 | Hoppe et al. | Sep 1994 | A |
5510616 | Seymour et al. | Apr 1996 | A |
6163158 | Moeller et al. | Dec 2000 | A |
20010000946 | Moeller et al. | May 2001 | A1 |
Number | Date | Country |
---|---|---|
41 19 821 | Dec 1992 | DE |
197 34 978 | Feb 1999 | DE |
0 434 457 | Jun 1991 | EP |
Number | Date | Country | |
---|---|---|---|
20060125468 A1 | Jun 2006 | US |