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(11) | EP 2 400 212 A2 |
| (12) | EUROPEAN PATENT APPLICATION |
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| (54) | LED lamp forming light distribution mode of approximate parallel optical array by using lenses |
| (57) A light-emitting diode (LED) lamp forming a light distribution mode of an approximate
parallel optical array by using lenses is provided. The LED lamp includes substrates
(1) for mounting LEDs (10), reflectors (2), a power source (5), and a top cover (6).
Each of the substrates has a condenser lens (11) at a front end of each of the LEDs
(10), and the condenser lenses (11) are used for converging beam angles of the LEDs
(10). The plurality of LEDs (10) is arranged in a matrix to form an approximate parallel
optical array. The reflectors (2) each have a curved surface (21) for performing reflection
and light controlling on light rays reflected and controlled by a curved wall. The
LED lamp realizes uniform lighting in the whole lighting range through performing
lens condensing once and reflection light controlling once, thereby achieving excellent
directivity of illumination and uniform brightness, and eliminating the glare phenomenon.
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BACKGROUND OF THE INVENTION
[0001] The present invention relates to a light-emitting diode (LED) lamp forming a light distribution mode of an approximate parallel optical array by using lens condensing, and a street lamp using the same, which belongs to the field of lighting technology.
[0002] In the wide areas of outdoor roads and squares, conventional lighting lamps are high-pressure sodium lamps or metal halide lamps. The high-pressure sodium lamps or metal halide lamps have a luminous efficiency of 60-80 lm/W, and have a service life of about 6000 hours (h). Currently, the LED lamps have a luminous efficiency of 100-120 lm/W, and have a service life of up to over 25000 h, and do not contain hazardous metal mercury. With the development of semiconductor technologies, such performance of the lamps has been increasingly enhanced. Thus, in recent years, energy-saving and environment-friendly LED lighting lamps have gradually become popular in the market.
[0003] The existing LED lighting lamps mainly have two implementations: one is placing an LED light source (briefly referred to as LED) within a conventional lamp; the other is laying out LEDs uniformly, and using a partial reflector or a partial lens for controlling the light. Unfortunately, the above two implementations still cannot overcome the defects of the conventional lighting lamps as follows. Firstly, the directivity of the illumination is poor. The regionality of the illumination is not obvious, that is to say, the lamp illuminates undesirable regions. Thus, in the case of providing the same luminous flux, the brightness of the region requiring the illumination is decreased. Secondly, the brightness is non-uniform, which results in a phenomenon of being bright at a close area and being dark at a distant area. As a result, the luminance of the distance area cannot reach the standard level, or the luminance of the close area is far beyond the standard level. Due to the non-uniform distribution of the illumination, a light source with a higher power and a higher luminous flux has to be adopted in design, so as to enable dark areas at both sides of the road and between two lamps reach the lighting standard level, thereby meeting the luminance requirements of the dark areas, which results in wastes of electric energy. Thirdly, the glare phenomenon cannot be eliminated. The so-called glare phenomenon refers to that when people observe a certain visual object, a dazzling light-emitting spot existing in the visual field may affect the observing effect, which makes people feel uncomfortable. Fourthly, the heat-dissipation problem is not well solved. Currently, about more than 80% of the energy consumption of the LEDs is converted into heat energy, and the semiconductor elements are not high temperature resistant. A lot of LEDs are concentrated in a relative small space, and the continuously increased heat makes the temperature of the LED chip become excessively high. If the generated heat energy cannot be dissipated timely, the luminous efficiency and the service life of the LED may be severely decreased under a high temperature. In most of the existing LED lamps, radiators are disposed horizontally, which have a poor heat convection effect.
[0004] The basic reasons for causing the above defects include that, the prior art cannot make full use of the light directionality of LEDs, cannot effectively and reasonably control the light rays generated by the LEDs, and cannot effectively dissipate the heats for the LED lamps.
BRIEF SUMMARY OF THE INVENTION
[0005] Accordingly, the present invention is directed to an LED lamp forming a light distribution mode of an approximate parallel optical array by using lenses, which has excellent directivity of illumination and uniform brightness.
[0007] In order to achieve the above objectives, the present invention adopts the following technical solutions.
[0008] An LED lamp forming a light distribution mode of an approximate parallel optical array by using lenses is provided, which includes substrates for mounting LEDs, reflectors, a power source, and a top cover.
[0009] A condenser lens is mounted in front of each of the LEDs, and the condenser lenses are used for converging beam angles of the LEDs.
[0010] The plurality of LEDs is arranged in a matrix to form the approximate parallel optical array.
[0011] The reflectors each have a curved surface for performing reflection and light controlling on light rays reflected and controlled by a curved wall.
[0012] The LED lamp further includes radiators, and each of the radiators has a plurality of heat dissipation fins arranged in a horizontal direction, in which the heat dissipation fins extend along a direction perpendicular to the ground surface.
[0014] Two substrates, two reflectors, and two radiators exist, which are symmetrically mounted on two sides of the LED lamp, and the radiators are mounted at an outer side, the substrates are mounted in the middle, and the reflectors are mounted at an inner side.
[0015] The curved surface of each of the reflectors has a vertical curvature for reflecting light rays from a plurality of LEDs along a vertical direction into a first predetermined range, and in the first predetermined range, a ratio of the number of LEDs distributed in each position to the number of LEDs along the vertical direction is in direct proportion to a square of a distance from the position to the LED.
[0016] The curved surface of each of the reflectors has a horizontal curvature for reflecting light rays from a plurality of LEDs along a horizontal direction into a second predetermined range, and in the second predetermined range, a ratio of the number of LEDs distributed in each position to the number of LEDs along the horizontal direction is in direct proportion to a square of a distance from the position to the LED.
[0018] The LED lamp provided in the present invention has excellent directivity of illumination, uniform brightness, can eliminate the glare phenomenon, and has desirable heat dissipation performance. In addition, the LED lamp has various advantages of a simple structure, being conveniently mounted, energy-saving, environmental friendly, and so on.
BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWING
[0019] The accompanying drawings incorporated in and forming a part of the specification, illustrate several aspects of the present invention, and together with the description serve to explain the principles of the invention.
FIG. 1 is a schematic view of a street lamp using an LED lamp according to the present invention.
FIG. 2 is a schematic structural view of an LED lamp according to the present invention.
FIG. 3 is a schematic structural view of a condenser lens of the LED lamp shown in FIG. 2.
FIG. 4 is a schematic view of a parallel optical array formed by a plurality of LEDs and the condenser lenses.
FIG. 5 is an enlarged schematic structural view of a reflector of the LED lamp shown in FIG. 2.
DETAILED DESCRIPTION OF INVENTION
[0020] As shown in FIG. 1, an LED lamp provided in the present invention is mounted on a street lamp with a height of H meters (m) (H is a natural number, which is the same below), for road lighting. It should be understood that, the LED lamp of the present invention may also be mounted in other indoor or outdoor lighting devices, for example, court lamps, square lamps, or landscape lamps. The street lamp is taken as an example below for demonstrating the structure of the LED lamp provided according to the present invention.
[0021] Referring to FIG. 1, a lighting range of each street lamp is a range having a length of 3.0H m along a length direction of the road (that is, an initial position is a line segment e, and a terminating position is a line segment f) and having a length of 1H m along a width direction (that is, an initial position is a line segment g, and a terminating position is a line segment h) with the street lamp as a center. The LED lamp is symmetric at left and right sides along the length direction of the road, so that the left side part of the street lamp is omitted here, and merely the right side part of the street lamp is discussed, that is, the range being 1.5H m long and 1H m wide on the right side of the street lamp along the length direction of the road. The attenuation of light rays is in direct proportion to a square of an illumination distance. Under the same illumination intensity, the farther away from the center of the light source of the street lamp, the smaller the brightness will be. It is assumed that a brightness of a near point A (which seems to be approximately the location of the street lamp) right under the LED lamp is 1 unit, so that a far point B 1.5H m away from the street lamp has a brightness of about 0.33 units. In order to enable the Point A and the Point B to have the same brightness, the luminous flux (illumination intensity) three times as much as that of the near point A is required at the far point B. Similarly, the illumination intensity of any point within the lighting range of the LED lamp can be acquired. In order to realize the uniform distribution of the illumination intensity within the lighting range, the light rays with the illumination intensity needs to be distributed on the light source, that is, the LED lamp, according to the lighting distance, and the light rays are reflected to the designated regions along a certain direction, so that the light rays are effectively controlled to be uniformly emitted to the required regions.
[0022] In order to meet the above requirements, the LED lamp of the present invention changes the divergence angle of the light source to form an approximate parallel optical array through performing condensing for a first time with a lens, and then realizes the required light controlling effects through performing reflection light controlling for a second time according to the directionality of the LED.
[0023] Referring to FIGs. 2 to 5, the LED lamp of the present invention is further described below in detail.
[0024] Referring to FIG. 2, the LED lamp of the present invention includes substrates 1, reflectors 2, radiators 3, a mounting frame 4, a power source 5, and a top cover 6. The substrates 1 further include a plurality of condenser lenses 11, and the mounting frame 4 further includes a front caulking 41, a retaining plate 42, and a rear caulking 43.
[0025] Referring to FIG. 3, a plurality of LEDs 10 is arranged on a substrate 1, and each LED 10 has a condenser lens 11 mounted on a front end thereof. The condenser lens 11 is preferably a cone-shaped or cup-shaped catadioptric lens, which is capable of performing transmission condensing right ahead, and a conical surface may collect all the side light and reflect the side light out, such that the overlapping of the two kinds of light (having the same angle) may obtain the perfect light ray utilization and desired light spot effect. The use of the condenser lens 11 may converge light emitting angles of the LED light sources, for example, a beam angle of an LED light source is about 120 degrees, and after passing through the condenser lens 11, the beam angle may be converged to about 10 degrees.
[0026] In practice, the condenser lens 11 may be made of silica gel, optical grade polymethylmethacrylate (PMMA), optical grade polycarbonate (PC), and glass. Taking the outdoor street lamp being irradiated by ultraviolet radiation, light transmittance, and easy production into consideration, the condenser lens 11 is preferably made of optical grade PC. However, other materials are also available according to actual demands.
[0027] As shown in FIG. 4, in order to make the LED lamp to generate parallel light with preferred directivity, a plurality of LEDs 10 may be arranged in a matrix to form a parallel optical array. By using this parallel optical array, diverging light having large angle may be irradiated to the reflector 2 in a light distribution mode approximate to parallel light, and then the reflector 2 performs precise light controlling.
[0028] Each of the reflectors 2 has a box-like overall shape, and has certain rigidity and stability itself. The reflector 2 includes a curved surface 21, a positioning mounting hole 22, and a light exit opening 23 for emitting the light rays, after being reflected by the reflector 2, to the exterior. The positioning mounting hole 22 and the light exit opening 23 are respectively located at two sides of the curved surface 21. The positioning mounting hole 22 is disposed at an edge of the reflector 2, and is used for directly connecting to the substrate 1, so as to effectively ensure the position precision of the substrate 1, thereby ensuring that the position on the reflector 2 where the light emitted from the LED 10 reaches does not bias.
[0029] The curvature of the curved surface 21 is determined according to the required lighting range and light control requirements on the uniform illumination for the LED lamp. Specifically, the curved surface 21 has a vertical curvature for reflecting light rays emitted by M LEDs along a quasi-vertical direction into a range from the near point A in the length direction of the road to the far point B in the length direction of the road, in which a ratio of the number of LEDs distributed to each position corresponding to the length direction of the road to the total number (that is, M) of LEDs along the quasi-vertical direction is in direct proportion to a square of a distance from the position to the LED. Similarly, the curved surface 21 has a horizontal curvature for reflecting light rays emitted by N LEDs along a quasi-horizontal direction into a range from a near point C in the width direction of the road to a far point D in the width direction of the road, in which a ratio of the number of LEDs distributed to each position corresponding to the width direction of the road to the total number (that is, N) of LEDs in the quasi-horizontal direction is in direct proportion to a square of a distance from the position to the LED. The above vertical curvature and horizontal curvature may be acquired through calculations according to the fundamental principle in the geometrical optics, which will not be further described here in detail. M and N are natural numbers, and the magnitudes of M and N are required to meet the light control precision requirements and the brightness requirements.
[0030] Taking FIG. 5 for example, it is assumed that the LED lamp needs to illuminate the range from the Point A to the Point B, and the reflector 2 needs to reflect light rays emitted by 4n LEDs (n is a natural number, which is the same below) connected in series. As mentioned above, in order to enable the Point A and the Point B to have the same brightness, the illumination intensity three times as much as that of the near point A is required at the far point B. Thus, the curved surface 21 reflects light rays emitted by the highest n LEDs to the Point A, and reflects light rays emitted by the other 3n LEDs to the Point B. Therefore, in one aspect, the light rays are ensured to cover the whole region from the Point A to the Point B, without illuminating any other undesirable region, thereby ensuring the desirable directionality of illumination; in another aspect, it is ensured that the illumination intensity at the Point B is the same as that of the Point A, that is, the brightness is uniform across the whole lighting range.
[0031] Each of the radiators 3 also achieves a supporting function. Each of the radiators 3 has a plurality of heat dissipation fins 31 arranged in a horizontal direction. The heat dissipation fins 31 extend along a direction perpendicular to the ground surface. After the air surrounding the radiator 3 is heated, the density of the air is reduced, so that the air rises upwards. The heat dissipation fins 31 in the radiator 3 are arranged along a direction consistent with the rising direction of the hot air, so that the circulating path is short, the heat convection is fast, and the heat dissipation efficiency is quite high.
[0032] The front caulking 41 on the mounting frame 4 is used for mounting the retaining plate 42, as well as for decoration. The retaining plate 42 is used for mounting the power source 5. The rear caulking 43 achieves a supporting function. In one aspect, the rear caulking 43 is used for cooperating with the front caulking 41 to mount the retaining plate 42, and in another aspect, the rear caulking 43 is used for mounting two reflecting enclosure members (further described later) symmetric on the left and right sides through the radiator 3. The LED lamp is mounted on a lamp post through a lamp post connecting mechanism on the rear caulking 43.
[0033] In the LED lamp of the present invention, the condenser lenses 11 are mounted at the front end of the LEDs 10, the substrates 1 and the condenser lenses 11 are mounted on the radiators 3, which are then assembled into the reflecting enclosure members together with the reflectors 2 and light transmissive plates. The two reflective enclosure members are symmetrically mounted on the rear caulking 43 through their respective radiators. The front caulking is mounted on the two radiators symmetric on the left and right sides through mounting holes at two sides thereof respectively. The retaining plate 42 is mounted on the front caulking and the rear caulking. That is, two substrates 1, two reflectors 2, and two radiators 3 exist, which are symmetrically mounted on the rear caulking 43 through the radiators. The substrates 1 are mounted at an outer side of the reflectors 2, and the radiators 3 are mounted at an outer side of the substrates 1. The power source 5 is configured at a middle position above the retaining plate 42, and the top cover 6 covers the power source 5. Through the above design solution, the LED lamp of the present invention has a simple overall structure and a reasonable heat dissipation structure, and further has a circular-arc-shaped external appearance transition, which thus has a small windward surface, thereby being more reasonable during the application in the actual environment.
[0035] The light from the condenser lens 11 is completely emitted to the whole reflection curved surface of the reflector 2, thereby realizing accurate light control effects. As shown in FIG. 5, the light rays emitted by the highest LEDs are condensed by the condenser lens 11, and are emitted to the curved surface 21 of the reflector 2. It is assumed that the luminous flux of each LED is A. The light rays from n LEDs are reflected by the corresponding regions on the reflector 2 and then reach the Point A (a distance to the LED is H), and the illumination intensity is k.nA/H2 (k is a proportion coefficient). The light rays from 3n LEDs are reflected by the corresponding regions on the reflector, and then reach the Point B (a distance to the LED is 1.5H), and the illumination intensity is k.(3nA)/[H2+(1.5H)2]≈k.nA/H2. Thus, the light intensity at the Point A and the Point B are the same. Similarly, the number of LEDs is distributed between the Point A and the Point B according to the above principle, so as to ensure the same light intensity at any position along the AB direction (a length direction of the road). Similarly, the same light intensity can be ensured at any position in the width direction of the road, thereby achieving the uniform illumination effects in a certain region.
[0036] Since no direct illumination of the light and no dramatic change of the brightness occurs, and the light control angle design of the reflectors 2 is utilized, the LED lamp of the present invention eliminates the unreasonable glare phenomenon, and satisfies the requirements of the using effects in the illumination environment, thereby having wide application prospects in the indoor and outdoor lighting.
[0037] The LED lamp forming a light distribution mode of an approximate parallel optical array by using lenses according to the present invention has been described above in detail. Any person skilled in the art who makes obvious modification on the present invention without departing from the substantial sprints of the present invention may be construed as infringing the patent rights of the present invention patent, so as to undertake the corresponding legal responsibility.
1. A light-emitting diode (LED) lamp forming a light distribution mode of an approximate
parallel optical array by using lenses, comprising: substrates (1) for mounting LEDs,
reflectors (2), a power source (5), and a top cover (6), characterized in that
a condenser lens (11) is mounted at a front end of each of the LEDs, and the condenser lenses (11) are used for converging beam angles of the LEDs;
the plurality of LEDs is arranged in a matrix to form an approximate parallel optical array; and
the reflectors (2) each have a curved surface (21) for performing reflection and light controlling on light rays reflected and controlled by a curved wall.
a condenser lens (11) is mounted at a front end of each of the LEDs, and the condenser lenses (11) are used for converging beam angles of the LEDs;
the plurality of LEDs is arranged in a matrix to form an approximate parallel optical array; and
the reflectors (2) each have a curved surface (21) for performing reflection and light controlling on light rays reflected and controlled by a curved wall.
2. The LED lamp as defined in claim 1, characterized in that the LED lamp further comprises radiators (3), each of the radiators (3) has a plurality
of heat dissipation fins (31) arranged in a horizontal direction, and the heat dissipation
fins (31) extend along a direction perpendicular to a ground surface.
3. The LED lamp as defined in claim 2, characterized in that the substrates (1) and the reflectors (2) are mounted on the radiators (3).
4. The LED lamp as defined in claim 3, characterized in that two substrates (1), two reflectors (2), and two radiators (3) exist; the substrates
(1), the reflectors (2), and the radiators (3) are symmetrically mounted on two sides
of the LED lamp; and the radiators (3) are mounted at an outer side, the substrates
(1) are mounted in the middle, and the reflectors (2) are mounted at an inner side.
5. The LED lamp as defined in claim 1, characterized in that the curved surface (21) of each of the reflectors (2) has a vertical curvature for
reflecting light rays from a plurality of LEDs along a vertical direction into a first
predetermined range, and in the first predetermined range, a ratio of a number of
LEDs distributed in each position to a number of the LEDs along the vertical direction
is in direct proportion to a square of a distance from the position to the LED.
6. The LED lamp as defined in claim 1, characterized in that the curved surface (21) of each of the reflectors (2) has a horizontal curvature
for reflecting light rays from a plurality of LEDs along a horizontal direction into
a second predetermined range, and in the second predetermined range, a ratio of a
number of LEDs distributed in each position to a number of the LEDs along the horizontal
direction is in direct proportion to a square of a distance from the position to the
LED.
7. A street lamp, characterized in that the street lamp uses the LED lamp as defined in claim 1.