CA2065577C

CA2065577C - Encapsulated light emitting diode and method for encapsulation

Info

Publication number: CA2065577C
Application number: CA002065577A
Authority: CA
Inventors: Jerry T. Pugh
Original assignee: Bayer Corp
Current assignee: Bayer Corp
Priority date: 1991-04-15
Filing date: 1992-04-08
Publication date: 2000-06-06
Anticipated expiration: 2012-04-08
Also published as: ATE147547T1; EP0509389A3; ES2095977T3; KR920020770A; TW222717B; DE69216456D1; JPH05145120A; DE69216456T2; EP0509389A2; KR100299720B1; US5122943A; EP0509389B1; GR3022530T3; AU634117B1; CA2065577A1

Abstract

A light emitting diode with reduced stray light includes a base with an active light emitting element mounted in the base. An epoxy envelope is mounted on the base. The envelope includes a conical side portion and a spherical dome portion. The envelope is encapsulated with optically absorbing material of low reflectivity. The optically absorbing material is in direct contact with the side portion of the envelope and part of the spherical dome portion leaving an exposed portion through which rays of light pass. The diameter d of the exposed portion is equal to: 2r[sin (x + arcsin (r/s/n))], wherein r is the radius of a spherical dome portion, x < arcsin (1/n) is the maximum angle between a surface normal and a ray emitted from the active light emitting element that strikes the envelope at the edge of the exposed portion of the spherical dome portion, s is the distance between the active light emitting element and the center of the spherical dome portion, and n is the index of refraction of the material of the epoxy envelope.

Description

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Dao~c~ou~d Of Tt~e Iaaqrentisa~n 1. F'ielc~ of the $alVextt3~n The present invention relates to a new and improved light emitting diode that is encapsulated with optically absorbing material to reduce stray light, and to a new and improved method for encapsulating a light emitting diode to reduce stray light.

2. Description of the Dack~und Art In designing blood glucose monitoring instruments, the direction of development has been toward smaller instruments that are lower in cost. To meet these goals, more than one function is designed into a single component.
This approach lowers the part count, reduces the size of the instrument and increases the reliability.
One example of this trend is the use of a light emitting diode (TaED) to replace the combination of an incandescent lamp, and an interference filter in the optical system of blood glucose monitoring instruments. examples , of instruments that use an LSD as a light source include the GLUCOMETER III manufactured by Miles, Inc., the ACCUCHECK manufactured by Boehringer Mannheim Gmb~T and the GLUCOSCAN

manufactured by Lifescara, Inc. Examples of devices using an LED in a readhead are to be found in United States F>atent Nos. 4,552,458:

and 4,676,653 and Europs:an Patent Application No. 83304306.6, filed July 26, 1983. LED light sources have also been used in other diagnostic instruments such as the instrument disclosed in United States Patent No. 4,755,058. The typical LED used as a light source in the readhead of a blood glucose monitoring system is the standard T-1 3/4 which can be purchased from manufacturers such as the ES Series made by Stanley Electric Co., Ltd. or the HLMP

Series from Hewlett-Packard.

One of the problems in using a standard LED as a light source in a blood glucose monitoring instrument is the stray light emitted by the LED. In a diagnostic instrument readhead it is preferable that the LED emission be generally collimated toward a small sample area. Rays emitted at wide angles are undesirable stray light that preferably are minimized or eliminated, since stray light in an optical system of a readhead instrument manifests itself as a background signal.

At least three procedures have been used 3o in instruments to control the stray light from an LED. One method is to ignore the existence of stray light. By ignoring the stray light, ~~~~ 3'~'~l

3 however, there can be a high level of instrument to instrument imprecision. Due to this imprecision, ignoring the stray light has not been considered an ~:cceptable method.
Another method of e:ontrolling stray light is to accept only a small solid angle of the emission from an LED.
Such an approach is used in the instrument described in United Stai:es Patent No.

4,676,653. This approach results in an instrument that uses only a small portion of the available light from the LED. This approach also reduces the magnitude of the available signal and can make the optical system more susceptible to noise.
Another approach is to use a shield to avoid the detection of the stray light. Such an approach is illustrated in European Patent Application No. 83304306.6. This approach does not shield the stray light flaring in directions other than in direct line with the shield. Commuter simulations have been performed that suggest 'that there is a significant amount of this light that flares in all directions after emission from an LED, and for this reason, shielding is not preferred.
SUMP~A3~Y Df TAE ~ielil'EN'fI~N
Briefly, the present invention is directed to a new and improved light emitting diode used in an instrument readhead such as in a blood glucose monitoring instrument. The LED may be of the standard type such as a T-1 3/4 plastic ~~~J..~..
LED lamp that includes a base with anode and cathode leads extending from the base to a location above the base. An active light emitting element is encapsulated within an epoxy envelope that is ~~ecurad on the base.

The epoxy envelope includes a conical side portion and a spherical dome portion or lens that extends above the ~;ide portion and encloses the envelope.

l0 To reduce the amount of stray light emitted by the active light emitting element, the side portion and part of the spherical dome portion are encapsulated by optically absorbing material. This material is placed in direct contact with 'the envelope leaving an exposed portion of the spherical dome portion.

Preferably, this encapsulation of the envelope is done such that the diameter of the exposed portion is equal to 2r[sin(x + arcsin (r/s/n))]

wherein r is the radius of the spherical dome portion, x < arcsin (1/n) is the maximum angle between a surface normal and a ray emitted from the active light emitting element that strikes the envelope at the edge of the exposed portion of the spherical dame, s is the distance between the active light emitting element and 'the center of the spherical dome portion, and n is the index of refraction of the epoxy material that defines the envelope.

5 BRIEF' DESCRIPTION OF THE DRh,NINC~S

Other objects and advantages of the present invention will become apparent upon reading the following detailed description and upon reference to the drawings in which:

FIG. 1 is a schematic illustration of a light emitting diode and the paths of different classes of rays of light;

FIG. 2 as a schematic illustration of a light emitting diode similar to FIG. 1 including optically absorbing material encapsulating the light emitting diode and illustrating the path of the different classes of rays of light.

FIG. 3 is a schematic illustration similar to FIG. 2 illustrating different dimensions of the light emitting diode; and FIG. 4 is a schematic illustration of the dimensions of different portions of the epoxy envelope of the light emitting diode of the present invention and the path and angles of light rays used to calculate the exposed , portion of the envelope uncovered by the optically absorbing material.

DESCRIPTION 0F' THE PREFERRED EI~BODIIriENT

Referring initially to FIG.1, there is illustrated a standard T-1 3/4 plastic LED lamp generally designated by the reference numeral 10. Only the elements of the LED 10 that are necessary for an understanding of the present invention will be described.

1~S 1660

6 The LED 10 includes a reflector dish 12 coined orito a cathode past 14. The cathode post 14 is part of a cathode lead 16 extending downwardly from the LED 10. The LED 10 also includes an anode post 18 that extends from the LED 10 'to an anode lead 20.

The LED 10 includes an LED chip or active light emitting element 22 electrically connected t~ the reflector dish 12 and the anode post 18. The active light emitting element 22 is positioned above a base 24 of 'the LED 10 and is encapsulated in or covered by an epoxy resin envelope generally designated by the reference numeral 26. The epoxy envelope 26 includes a tapered or conical side portion 28 and an upper spherical dome portion 30. The base 24 encloses the lower end of the epoxy envelope 26, and the spherical dome portion 30 encloses the upper end of the epoxy envelope 26. In addition, the upper spherical dome portion 30 functians as a magnifying lens for the rays of light emitted from the active light emitting element 22. Although a T-1 3/4 LED

lamp is illustrated and disclosed, it is intended to be recognized that other LEDs with other shaped domes, for example, a parabolic surface of revolution, are included in this invention as long as the diameter d of the shape limits the angle x to less than arcsin (1/n) .

As best illustrated in FIG. 1, the light rays emanate from the active light emitting

7 element 22, strike 'the various optical surfaces, and are refracted by 'the epoxy resin envelope 26. A computer simulation for an LED

without a reflecting cone was used to determine that the rays emitted from the active light emitting element 22 can be grouped into four classes. Class 1 rays are refracted by the spherical dome portion 30 of the epoxy resin envelope 26. Class 1 rays make up about 29% of the total rays, and are the most useful rays in an instrument readhead application since they remain generally collimated at some distance from the LED 10. Class 2 rays are refracted by the spherical dome portion 30 of the epoxy resin envelope 26 after first being internally reflected by the side portion 28 of the epoxy resin envelope 26. Class 2 rays make up about 19% of the total rays. Class 2 rays are not useful in an instrument.readhead application as they form a ring which diverges widely upon leaving the LED 10.

Class 3 rays pass through and are refracted by the side portion 28 of the epoxy resin envelope 26. Class 3 rays make up about 28% of the total rays, and are not useful as they also form a wide diverging background upon leaving the LED 10.

Class 4 rays are internally reflected by the epoxy resin envelope 26 and make up the remaining 24% of the total number of rays. As with class 2 and 3 rays, class 4 rays are not ~~~_-~~N~fl ~'~~~,~~~

8 useful in an instrument readhead application since they exit the back of the LED 10.

In order to maximize the effectiveness of an LED 10 in an instrument readhead, it is desirable to prevent the class 2, class 3 and class 4 rays from exiting the LED 10. In the present invention, this is accomplished by encapsulating the LED 1o with an encapsulating material 32 (FIGS.2-4). The encapsulating material 32 is preferably an optically absorbing material of a low reflectivity such as black plastic or black painted material and can be a sleeve that is slipped onto the LED

or it can be molded onto the LED 10. The encapsulating material 32 completely surrounds and is in direct contact with the side portion 28 of the epoxy resin envelope 26. In addition, the encapsulating material surrounds and is in direct contact with at least a portion of the spherical dome portion 32 leaving an exposed portion 34 through which class 1 rays may pass. In a preferred embodiment, the encapsulating material 32 may include snaps or notches 36 that facilitate the retention of the encapsulated LED 10 in an optical readhead of an instrument.

The encapsulating material 32 prevents the class 2, class 3 and class 4 rays from exiting the LED 10. As an example, the encapsulating material 32 absorbs the class 3 rays that would otherwise be refracted through the side portion 28 of the epoxy resin envelope 26 at the point r~s 1660 s ~~ ~y ~~~ ~ s t~ ~ :.~ -3

9 a in FIG: 2. Also, the encapsulating material 32 frustrates the total internal reflection of class 2 and 4 rays at point b and point c, respectively, in FIG. 2. This is accomplished by lowering the internal reflectance from 100%

to the reflectance of the encapsulating material 32>

The result of the use of the encapsulating material is that only class 1 rays as illustrated in FIG. 2 pass through the exposed portion 34 of the epoxy resin envelope 26, and these are the most useful and effective light rays emitted by the LED 10. Thus, the encapsulated LED 10 provides the best light source for an instrument readhead by preventing unwanted rays from exiting the LED 10.

Significantly less aperturing is required in the illumination optics of an instrument readhead in which the encapsulated LED 10 is incorporated. This less apexturing allows more of the class 1 rays to illuminate a sample.

For example, a computer simulation has shown that a 2.5 to 3 fold increase in signal level is possible by encapsulating a LED 10.

In order to insure that the class 2, class , 3 and class 4 rays are prevented from exiting the LED 10, the diameter d (FIGS. 3 and 4) of the exposed portion 34 of the epoxy resin envelope 26 must be calculated and maintained during encapsulation. The diameter d of the exposed portion 34 must be sized such that the rays emitted from the active light emitting y ~'7 ,7 rv L. r !°
element 22 that strike the surface of the epoxy resin envelope 26 inside this diameter (for example, ray 22-b in FIG. 3) are not internally reflected, but are refr<zcted out of the epoxy 5 resin envelope 26 (for example, the ray b-c in FIG. 3). In order to insure that a ray is not internally reflected, the angle the ray makes with a surface normal 38, such as the angle x in FIGS. 3 and 4, must be less than a critical

10 angle given by the formula: sin(x) <1/n; where n is the index of refraction of the epoxy material of the envelope-26. If the worse case ray 22-b-c shown in FTG. 4 is considered, from the triangle b-o-a the formula can be written:

d/2 = r [sin (180-z)], but 180-z = x + y, therefore, d = 2r[sin (x + y)]. From the law of lines we know: rsin (x) = s [sin (y)], or:

y = arcsin [r (sin(x)/s)], and substitution gives: d = 2r(sin (x + arcsin (r/s/n/))], where x < arcsin (1/n). In a typical example with r = .079 inch, s = .123 inch, and n = 1.5, the equation results in x = 41.8 degrees and d - 0.146 inch. Through this calculation, the diameter d of the exposed portion 34 of the preferred encapsulated LED 10 can be determined, and encapsulated light emitting diodes 10 can be manufactured in quantity with consistency. The light emitting diodes 10 may then be used in instrument readheads providing the best available light source.

rIS 1660

Claims

The embodiments of the invention in which an exclusive property or privilege is claimed are defined as follows:

1. A light emitting diode encapsulated for reducing stray light, comprising:
a base (24) and an active light emitting element (22) mounted on said base;
an envelope (26) with a conical side portion (28), said conical side portion mounted on said base (24);
said envelope including a spherical dome (30) and extending from said conical side portion (28);
and encapsulating material (32) surrounding said conical side portion (28) and part of said spherical dome end (30) with an exposed portion of said spherical dome end (34) uncovered by said encapsulating material (32);
wherein said light emitting element (22) is located under the center of the spherical dome end (30) and the diameter d of the exposed portion of said spherical dome end (34) is equal to or less than 2r ~ [sin (arc sin (1/n) + arc sin (r/ (sn)))], wherein r is the radius of said spherical dome end (30), s is the distance between said active light emitting element (22) and the center of said spherical dome end (30), n is the index of refraction of the material of said envelope, and the maximum angle x between a surface normal and a ray emitted from the active light emitting element (22) that strikes the envelope at the edge of the exposed portion of the spherical dome (34) is defined as x = arc sin(1/n).

2. A method of reducing stray light emitted from a light emitting diode, wherein said light emitting diode includes an active light emitting element (22) located under the center of the spherical dome end (30) and mounted within an envelope (26) including a side portion (28) and a spherical end portion (30), the method comprising the steps of:
encapsulating said side portion (28) of said envelope (26) with material of low reflectivity;
and encapsulating a portion of said spherical end portion (30) of said envelope (26) with said material of low reflectivity leaving an exposed portion (34);
wherein the step of encapsulating a portion of the spherical end portion (30) of said envelope (26) further includes leaving said exposed portion (34) with a diameter d equal to or less than 2r ~ [sin (arc sin (1/n) + arc sin (r/ (sn)))] wherein r is the radius of said spherical dome end (30), s is the distance between said active light emitting element (22) and the center of said spherical dome end (30), n is the index of refraction of the material of said envelope, and the maximum angle x between a surface normal and a ray emitted from the active light emitting element (22) that strikes the envelope at the edge of the exposed portion of the spherical dome (34) is defined as x = arc sin(1/n).

3. The method according to Claim 3, wherein the material for encapsulating said side portion of said envelope (26) and said portion of the spherical end portion (30) of said envelope (26) is an optically absorbing material.