Title: Semi-enclosed gel delivery device
Abstract: A dispenser of actives having a linear release rate may be achieved by providing a volatile containing gel system wherein the gel system is proportioned in specified dimensional ratios, so that the sum of the rate of volatile release from directly exposed areas of the surface of the gel system and the rate of volatile release from areas of the surface of the gel system which are not in direct exposure to the atmosphere remains essentially constant through out the life of the dispensing device.
Patent Number: 6,994,270 Issued on 02/07/2006 to Wongosari,   et al.
| Inventors:
|
Wongosari; Anita (San Luis Obispo, CA);
Liptrot; Michael C. (Cambridge, GB);
Varanasi; Padma Prabodh (Racine, WI)
|
| Assignee:
|
S.C. Johnson & Son, Inc. (Racine, WI)
|
| Appl. No.:
|
712507 |
| Filed:
|
November 13, 2003 |
| Current U.S. Class: |
239/34; 239/41; 239/42; 239/47; 239/55; 239/58 |
| Current Intern'l Class: |
A24F 25/00 (20060101); A61L 9/04 (20060101) |
| Field of Search: |
239/60,55,47,35,34
|
References Cited [Referenced By]
U.S. Patent Documents
| 2733956 | Feb., 1956 | Wenner.
| |
| 3239145 | Mar., 1966 | Russo.
| |
| 3910495 | Oct., 1975 | Cummings et al.
| |
| 4157787 | Jun., 1979 | Schwartz.
| |
| 4809912 | Mar., 1989 | Santini.
| |
| 5060858 | Oct., 1991 | Santini.
| |
| 6631852 | Oct., 2003 | O'Leary.
| |
| Foreign Patent Documents |
| 778600 | Jul., 1957 | GB.
| |
| 1359447 | Jul., 1974 | GB.
| |
| WO 00/2443/4 | May., 2000 | WO.
| |
Primary Examiner: Sherbel; David A.
Assistant Examiner: Hogan; James S.
Parent Case Text
RELATED APPLICATION
This application claims the benefit of U.S. Provisional Application Ser. No.
60/426,845, filed Nov. 15, 2002.
Claims
What is claimed is:
1. A semi-enclosed gel system for release of volatile materials, wherein the
dimensions of the gel system, in the x, y, and z dimensions, are such that:
xi/yi>1.5, a.
Hi/zi>2.0, b.
xF/yF>2.0, c.
##EQU4##
wherein: A
D=Surface Area of the gel that is directly exposed to ambient
flowing air
A
P=Area available for permeation of vapors generated within the enclosure
##EQU5##
##EQU6##
wherein: x
i=the longest dimension measured in the x direction of the
projection of the directly exposed region of the gel system in the x-z plane at
the initiation of volatilization;
y
i=the longest dimension measured in the y direction of the projection
of the directly exposed region of the gel system in the x-y plane at the initiation
of volatilization;
z
i=the longest dimension measured in the z direction of the projection
of the directly exposed region of the gel system in the x-z plane at the initiation
of volatilization;
H
i=the longest dimension measured in the z direction of the projection
of the entire gel system in the x-z plane at the initiation of volatilization;
x
F=the longest dimension measured in the x direction of the projection
of the directly exposed region of the gel system in the x-z plane at the end of volatilization;
y
F=the longest dimension measured in the y direction of the projection
of the directly exposed region of the gel system in the x-y plane at the end of volatilization;
z
F=the longest dimension measured in the z direction of the projection
of the directly exposed region of the gel system in the x-z plane at the end of
volatilization; and
H
F=the longest dimension measured in the z direction of the projection
of the entire gel system in the x-z plane at the end of volatilization.
2. The semi-enclosed gel system of claim 1, wherein:
a. the ratio of final to initial values of A
D is greater than 0.65;
b. the ratio of final to initial value A
p is less than 4.0; and
c. the aspect ratio of the cross-section of the gel is greater than 1.5.
3. The semi-enclosed gel system of claim 2, wherein said volatile material is
selected from the group consisting of materials employed for air freshening, insect
control, and odor abatement.
4. The semi-enclosed gel system of claim 2, wherein said volatile material is
a fragrance.
Description
BACKGROUND OF THE INVENTION
The present invention relates to dispensers of volatile materials, which comprise
a gel-type solid or semi-solid mass of material which is designed to release the
maximum amount of volatile material over time, with a near-linear release rate.
That is, the rate of release of volatile material is essentially uniform over the
life of the dispenser.
The public is familiar with a number of solid or gel type air fresheners or dispensers
of volatile materials. Most familiar are those which are sold to the public as
Glade® air fresheners, produced by S. C. Johnson & Son, Inc., Racine, Wis.,
and Renuzit® air fresheners, a product of Dial Corporation, of Scottsdale,
Ariz. While other dispensers of volatile materials, and air fresheners, are known,
such as liquids incorporating wicks to assist in the evaporation of the liquid,
and materials which may be heated to volatilize fragrances or other vaporizable
components, the present invention is specifically directed to dispensers of volatile
materials wherein a fragrance or other volatile active is encompassed within a
solid or semi-solid material and is released over time by vaporization, to provide
a pleasing fragrance, to release a pesticide or insect control material, to counter
offensive odors, or to serve some other purpose. Aside from the problem of evaporation
of volatile material from the dispenser prior to sale to the consumer, a problem
associated with such dispensers is the drying, or shriveling, of the gel as the
active material is released, resulting in an unattractive mass of hardened and
emptied material to be disposed of, while the active, or volatile material is dispensed
from the gel at an uneven or variable rate. That is, the fragrance or other active
material is dispensed from the gel at a high rate upon initial exposure to the
atmosphere, and more slowly as time passes, so that near the end of the life span
of the dispensing device and its contained material, the volatile material is being
released at rate which is much lower than the initial rate of release.
BRIEF SUMMARY OF THE INVENTION
We have found that a near-linear release of actives from a gel type dispenser
of active materials may be achieved by providing the gel in a specific configuration,
whereby delivery of the active to the atmosphere is enhanced.
Such systems may be classified, generally, as either a semi-enclosed gel, or
an open gel system. For understanding, we have defined a semi-enclosed gel system
as being one in which only part of the gel surface is exposed directly to flowing
ambient air, and an open gel system as being one in which essentially the total
available gel surface is exposed to the ambient air. The present invention addresses
semi-enclosed gel systems.
The total release rate from an open gel (TRR
OG) is proportional to
the surface area of the entire gel, as given by the following expression:
TRROG=K*Co*AD (1)
Where C
o=Concentration of the active at the gel surface;
- K=Mass Transfer Coefficient; and
- AD=Surface Area of the gel in a the completely open device.
Based on Equation 1, a close to zero-order release (i.e., constant release
rate with time) can be obtained in a completely open gel system only if the surface
area of the gel A
D remains constant or is permitted to change only by
a small fraction during the entire life of the product. Thus, by careful control
of the configuration of the gel surface one is able to achieve a zero-order release
of active materials from the gel system, providing a relatively constant release
rate of the active material from initial opening until final disposal upon completion
of evaporation of the active material.
However, in the case of a semi-enclosed gel (as opposed to an open gel),
parameters in addition to surface area of the gel will influence the total release
rate from the device. This observation is based on analysis of semi-enclosed gels.
Based on our analysis, the total release rate from a semi-enclosed gel (TRR
SEG)
is given by the formula:
##EQU1##
Where,
- AD=Surface Area of gel that is directly exposed to ambient
flowing air;
- AP=Area available for permeation of vapors generated within
the enclosure;
- G=Gap Height;
- H=Gel Height;
- D=Diffusion Coefficient.
A careful examination of Equation 2 suggests that two parameters, namely, A
D
and A
p, play an important role in determining the total release rate
from a semi-enclosed gel. The first term on the right hand side of equation 2 depicts
the direct evaporative contribution from the exposed part of the gel to the total
release rate. The second term denotes the permeation contribution of the vapors
generated within the enclosure to the total release rate. Usually, the direct evaporative
contribution decreases with time due to a decrease in the value of A
D with
time. However, the permeation contribution increases with time due to an increase
in the value of A
P with time (in fact, in some cases where the aspect
ratio of the cross-section of the gel is close to 1, A
P can go through
a maximum). These counteracting effects of the first and second terms of equation
2 can lead to a close to a zero-order release rate, if applied as set forth hereinafter.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 illustrates the exterior container of a gel type dispenser of volatile
materials in accordance with the present invention, in perspective view.
FIG. 2 illustrates the planar relationship of the coordinates of a gel system
in accordance with the present invention.
FIG. 3 illustrates the relationship between the container and the gel system
of the present invention, showing the areas of release of the volatile material,
i.e. the flux lines of the volatile material released.
DETAILED DESCRIPTION OF THE INVENTION
The present invention is related to gel type dispensers of active, or volatile
materials, of the type commonly employed for air freshening, insect control, odor
abatement, and the like. As shown in FIG. 1, such a dispenser (
1), commonly
comprises a base (
2), and a cover or closure member (
3) in which
the base contains a volatile material, for example an air freshening deodorizer
or fragrance, and in which the closure or cover is manually displaceable with respect
to the base to provide means for control of the effective rate of volatilization
or evaporation of the active material. Such cover or closure member commonly may
be positively locked with respect to the base, as shown in FIG. 1, to prevent unintended
evaporation or volatilization of the active material. After opening of the closure
member to expose the contained gel, the cover may be adjusted relative to the base
to permit substantial control or variation of the rate of volatilization of the
gel. Said base and cover may preferably be of a molded plastic material, although
other materials may be utilized. The container may further comprise support members
or posts, around which the gel member is molded or formed, which members or posts,
which may be singular or plural, provide support and strength to the gel material
in the container. The gel materials to which the present invention applies are
well known to practitioners of the art, as are the methods of manufacture and positioning
in a container such as shown in FIG. 1, and need not be discussed in greater detail
for the purpose of this invention. The provision of active or volatile materials,
and the choice thereof for the purposes of the dispensing devices of this invention,
are also well known, and as such need not be discussed further. Rather, the present
invention is directed to the relationship of the dimensions of the gel or solid
actives containing material of the device.
To achieve a constant (zero-order) release rate for the volatile within a gel
system, it is useful to consider the three dimensional configuration of the actives
containing material (hereinafter the gel system), as shown in FIG. 2. In FIG. 2,
dimensions x, y, and z are illustrated, having an origin point (0,0,0) at the intersection
of said dimensions, wherein the gel system should be placed in such a way that
it completely lies in the first quadrant of the x, y, z coordinate system and one
point touches the origin point (0,0,0). The dimensions x, y, z and other parameters
are defined thusly:
- xi=the longest dimension measured in the x direction of the
projection of the directly exposed region of the gel system in the x-z plane at
the initiation of volatilization;
- yi=the longest dimension measured in the y direction of the
projection of the directly exposed region of the gel system in the x-y plane at
the initiation of volatilization;
- zi=the longest dimension measured in the z direction of the
projection of the directly exposed region of the gel system in the x-z plane at
the initiation of volatilization;
- Hi=the longest dimension measured in the z direction of the
projection of the entire gel system in the x-z plane at the initiation of volatilization;
- xF=the longest dimension measured in the x direction of the
projection of the directly exposed region of the gel system in the x-z plane at
the end of volatilization;
- yF=the longest dimension measured in the y direction of the
projection of the directly exposed region of the gel system in the x-y plane at
the end of volatilization;
- zF=the longest dimension measured in the z direction of the
projection of the directly exposed region of the gel system in the x-z plane at
the end of volatilization; and
- HF=the longest dimension measured in the z direction of the
projection of the entire gel system in the x-z plane at the end of volatilization.
As illustrated in FIG. 3, evaporation or flux of the volatile material may take
place, in the direction of arrow
5, from the surface area not directly exposed
to the atmosphere by movement of the cover
3 away from base
2, through
gap
4, in the area defined as A
P, the Permeation Area, i.e.,
the area that is not directly exposed to the atmosphere, but is able to volatilize
active material. Of course, evaporation or flux of volatile material also occurs
through the gap,
4, in the direction of arrows
6 and
7, from
the surface area which is directly exposed to the atmosphere, A
D.
To maintain a release rate that does not deviate significantly from zero-order
release, the following ratios must be achieved:
xI/yI>1.5, preferably >2.0, and
most preferably >5.0; (1)
HI/zI>2.0, preferably >4.0, and
most preferably >5.0; (2)
xF/yF>2.0, preferably >5.0, and
most preferably >5.0; (3)
##EQU2##
wherein: A
D=Surface Area of the gel that is directly exposed
to ambient flowing air
- AP=Area available for permeation of vapors generated within
the enclosure
##EQU3##
The preferred way to achieve a close to zero-order release rate is by ensuring
that the percentage changes in both A
D and A
p during the
life of the product are confined to certain limits. The following table shows the
percentage changes associated with the parameters A
D and A
p during
the life of the product in the case of the present invention and a conventional
Renuzit® air freshener.
| |
|
| |
Direct Evaporation |
Permeation |
|
| |
Area (AD) |
Area (AP) |
| |
|
|
Final/ |
|
|
Final/ |
Aspect |
| |
Initial |
Final |
Initial |
Initial |
Final |
Initial |
Ratio |
|
| Invention |
32.39 |
23.75 |
0.7333 |
6.88 |
26.6 |
3.866 |
1.75 |
| Renuzit |
26 |
9 |
0.3462 |
4.62 |
31.84 |
6.892 |
1 |
|
Based on the above table, we believe that by adhering to the following conditions,
release rates that do not depart significantly from zero-order can be achieved:
- the ratio of final to initial values of AD should be greater
than 0.65;
- the ratio of final to initial value Ap should be less than
4.0; and
- the aspect ratio of the cross-section of the gel should be greater than 1.5.
Additional experiments demonstrated that by eliminating the permeation
flux by covering the surface of that part of the gel that lies within the enclosure,
it is feasible to have a zero-order release behavior for an extended period of
the life of the product. This happens because the gel that lies within the enclosed
region of the device serves as a reservoir to supply gel to the direct evaporation
region so as to maintain the fractional change in its surface area to smaller values
(a condition required for zero-order behavior according to equation 1).
*