JPH0359402B2 - - Google Patents

Description

[Detailed description of the invention]

The present invention relates to a reflector for lighting equipment, and more particularly to a reflector that is installed with its focal point aligned with the light source position and used to reflect a portion of the luminous flux emitted from the light source toward the front. It is. FIG. 1 is a cross-sectional view of an illumination lamp including a conventional reflecting mirror 1 of this type, including the optical axis Z--Z. Conventionally, the above-mentioned reflecting mirror 1 is generally configured in the shape of a paraboloid of revolution,
A part of the light beam emitted from the light source 2 provided at the focal point F is reflected in parallel to the optical axis Z-Z. A lens 3 is attached to cover the front opening of the reflecting mirror 1 in order to obtain a desired light distribution pattern by dimming the parallel light beam reflected as described above. FIG. 2 is a partial front view of the lens 3. In Fig. 1, the light emitted from the light source 2 and reflected by the reflecting mirror 2 is shown by arrows A, R ~ and I', R' ~ T'.
It is shown. Although not shown, in addition to the above-mentioned arrows, there is also light emitted directly forward (to the left in the figure) from the light source 2. As the lens 3, a spherical prism having a large number of concave spherical surfaces or a semicylindrical prism having a large number of concave cylindrical surfaces is generally used. Arrows 1 to 1 in FIG. 1 indicate a state in which a light beam reflected parallel to the optical axis Z-Z is scattered by the prism surface 3a. Figure 3 shows the light distribution pattern when a screen (not shown) is placed perpendicular to the optical axis Z-Z when a lens formed with a spherical prism is used;
H is the horizontal axis and V-V is the vertical axis. The luminous intensity distribution on the horizontal axis H-H above is the fourth
As shown in the figure, the brightness reaches its maximum in the center and decreases as it approaches the periphery. Although this tendency is common to this type of illumination lamp that has been generally used in the past, it is difficult to control this luminous intensity distribution curve as desired based on the design intention. FIG. 5 shows a light distribution pattern when a lens having a semicylindrical prism is used. Even when a semicylindrical prism is used, it is difficult to control the light intensity distribution curve as desired. Although there are some lamps for which conventional light distribution patterns such as those shown in FIGS. 4 and 5 described above are convenient, there are also cases where such light distribution patterns are not optimal. For example, if this is used in a stop light for a car, the maximum brightness area is in the center of the lens, so it will easily attract the attention of following cars, but if this maximum brightness area is much brighter than the surrounding area, it will be even better. desirable. Conventionally, in order to bring the light distribution of this type of illumination light closer to the desired pattern, various attempts have been made to design the prism provided in the lens 3, but thick prisms or prisms with complicated shapes are expensive to manufacture. Moreover, it is impossible to control the light distribution pattern as desired by the prism shape. Furthermore, as shown in FIG. 1, conventional illumination lights of this type have a large depth dimension L, so they require a large installation volume and are susceptible to installation restrictions. In order to solve this problem, when the lens 3 shown by the solid line is moved back to the position 3' shown by the imaginary line, the light emitting area of the lens is reduced. In view of the above-mentioned circumstances, the present invention has been made to eliminate the drawbacks of conventional devices.The purpose of the present invention is to enable the light distribution characteristics to be set arbitrarily. The luminous intensity of the area can be made more than twice the luminous intensity of other parts, and even when the depth dimension of the lamp is set shallow, it is possible to construct a lamp with a large light emitting area using a simple lens. To provide a reflector for a lamp which has a high effective utilization rate of light emitted from a light source. In order to achieve the above object, the reflector for a lamp of the present invention has an angle θ with respect to the optical axis of the light incident from the light source toward the reflecting surface, a luminous intensity I ₀ of the light source, and an angle α of the reflected light with respect to the optical axis. In the range of α<0, I ₀ cosθ=Asinα−(B+Aα)cosα+C ₁ ……
(1-1) In the range of α≧0 −I ₀ cosθ=Asinα−(B+Aα)cosα+C ₂
...(1-2) While maintaining the following relationship, the coordinates (x ₁ , z ₁ ) of the point where the light emitted from the light source is incident at an angle θ to the optical axis
And the coordinates (x ₂ ,
z ₂ ) is x ₂ = x ₁ tan (θ − α / 2) − z ₁ / cot (θ + Δθ) + tan
(θ−α/2)……(2) z ₂ =−{x ₁ tan(θ−α/2)−z ₁ }/1+tan(θ+Δ
θ)×tan(θ−α/2)……(3) It has a curved surface formed by rotating the continuous curve expressed by In addition, it is characterized in that the angle α is configured to decrease as the angle θ increases. FIG. 6 is an explanatory diagram of the angle θ and the angle α shown in the above formula. Let us consider the light that enters the reflective mirror surface M from the light source position F as shown by arrow W. Point A is the point of incidence,
Z′ shown by a dashed-dotted line passes through the incident point to the optical axis Z-
It is a line parallel to Z. The arrow y indicates the reflected light at the incident point. In this case, the angle θ of the light incident from the light source toward the reflective surface (arrow wa) with respect to the optical axis, and the angle α of the reflected light (arrow y) with respect to the optical axis are as shown in the figure. When the above angle θ is further increased by a small angle Δθ,
The incident light becomes as shown by the arrow T, and is reflected at the incident point as shown by the arrow S. Z'' is a line that passes through the incident point L and is parallel to the optical axis Z-Z. The imaginary line arrow Y' is added for convenience of explanation, and the line passes through the incident point L and is parallel to the reflected light arrow Y. is an imaginary line drawn at an angle α to the line Z″
are doing. As mentioned above, the light incident on the reflective surface M changes from arrow wa to arrow ta, and as a result, the angle it makes with the optical axis becomes θ.
When the angle increases from θ to θ+Δθ, compared to the angle α that the reflected light arrow Y makes with the optical axis, the angle that the reflected light arrow SO makes with the optical axis becomes α+Δα, which changes by Δα. In the reflecting mirror of the present invention, the angle θ and the angle α are
The outward direction with respect to the optical axis Z-Z is expressed as positive, and the inward direction is expressed as negative. In the configuration of the present invention, the fact that the angle α increases as the angle θ increases means that the value of Δα in FIG. 6 is positive. In other words, the arrows Y and X are not completely parallel, but are slightly in the direction of diffusion. Generally, the focal point of a concave mirror refers to the point where the incident parallel light beams intersect; however, since the reflecting surface M of the present invention is configured as described above, even if the parallel light beams are incident, they are completely focused on one point. Does not focus light. Therefore, in the reflecting mirror of the present invention, the focal point refers to the point where the parallel incident light beams are focused and have the maximum density. Next, one embodiment of the present invention will be described with reference to FIGS. 6 to 9. As shown in FIG. 6, the coordinates of the incident point F at the angle θ are (x ₁ , z ₁ ), and the coordinates of the incident point L at the angle θ+Δθ are (x ₂ , z ₂ ). Then, the relationship between these coordinates is maintained as shown in equations (2) and (3) above, and the curve M is obtained using an analytical mathematical method as detailed below. This curve M is a figure on the Z-X plane that is later rotated around the Z axis to determine the three-dimensional shape of the reflecting surface. That is, if we consider the case of finding a reflector shape to obtain a circular light distribution pattern with luminous intensity distribution I=f(α), the above I=f(α) represents the desired light distribution as a function of α. In this way, first the value of α is determined by design, and then θ is determined as described later. Using this θ, the above (2),
The shape of the reflecting mirror can be found from equation (3). It is assumed that the light source is a point light source located at a focal point F. Although the illustrated angle θ is a variable, its minimum value is not a value. The reason is that a bulb socket (not shown) for mounting the light source bulb is provided near the intersection of the curve M and the Z-axis, so the intersection of the curve M and the Z-axis (the center of the reflector) is located near the reflector. This is because it cannot function as a The minimum value of θ above is set as θ ₀ , and using this as an initial value, the curve M is sequentially drawn while increasing the minute angle Δθ. When the shape of the reflector is determined by design by applying the present invention, the initial value θ ₀ of the incident angle θ becomes tan ⁻¹ (x ₀ /z ₀ ). The point (x ₀ , z ₀ ) is the initial value of the reflector on the XZ plane. In actual design work, the value of the above angle θ ₀ is given as a design condition. Further, the value of Δθ is a minute value that can be arbitrarily set by the designer, and the curve M is obtained in the order of missing points and missing points while increasing the incident angle by this minute angle Δθ. In this case, it is appropriate that the angle Δθ be a small angle of, for example, 0.01°. For example, while increasing the incident angle by Δθ=0.01°,
If you try to cover = 60°, you will need to repeat the calculation about 6000 times. Although it is extremely difficult to perform such calculations manually, they can be performed quickly and easily using an electronic computer. Letting ΔWin be the solid angle of the light that enters a minute portion (curve) on the reflector from the light source located at the focal point F in Figure 6, the solid angle ΔWin is ΔWin=2π(cosθ−cos(θ+Δθ) ) ...(4) becomes. Also, the solid angle ΔWout of the light reflected by a minute part (curve) on the reflector is ΔWout = 2π (cos α − cos (α + Δα)) ... (5) Therefore, the light source luminous intensity I ₀ and the light intensity distribution I=f(α)
From equations (4) _and (5), _the relationship between
)...(6) Here, if Δθ and Δα are made infinitely small, I=I ₀ sinθ/sinα×dθ/dα...(7) is obtained. Let the light intensity distribution I be a linear function of the output angle α of the emitted light: f(α)=Aα+B (8). When the relationship between the incident angle θ and the exit angle α is determined from the above equations (7) and (8), −I ₀ cos θ=Asin α−(B+Aα) cos α+C (9) is obtained. However, C is an integral constant and is determined by the initial conditions of the design. Using equations (8) and (9) above, we obtain the coordinates of point (x ₁ , z ₁ ) and point (x ₂ , z ₂ ) shown in Figure 6. Equations (2) and (3) are obtained. A curve M is determined based on these equations (2) and (3), and when this curve M is rotated around the optical axis Z-Z, a rotating surface with the optical axis as the central axis is obtained. A reflecting mirror 4 (FIG. 7) is constructed in which all or part of this rotating surface serves as a reflecting surface. 5 shown in the same figure
is a lens attached to the front surface of the reflecting mirror 4. Then, a desired light distribution curve is set as shown in FIG. 8A. FIG. 9 shows the light distribution pattern. In order to obtain the desired light distribution characteristics shown in these charts, the above-mentioned curve M is calculated as follows. Points a, b to e shown in FIG. 7 are points of incidence of light emitted from the light source 2, respectively. Arrow R _a
~R _e indicates the reflected light at each of the above incident points. For convenience of discussion, first, the optical path drawn below the optical axis Z-Z in this figure will be described. The angles that the reflected lights R _a to R _e make with respect to the optical axis Z-Z are α _a to α _e , respectively. The above reflection angles α _a to α _e are plotted on the horizontal axis of FIG. 9, and the maximum luminous intensity I ₁ and the luminous intensity I ₂ in the peripheral area are set. The line connecting the center and periphery is I=f(α)=Aα+
It is represented by B. In this formula, A means the slope of luminous intensity, and A=I ₁ −I ₂ /α _e −α _a . B means the minimum luminous intensity in the periphery, and B=I ₁ −Aα _e . I ₀ in the above equations (1-1) and (1-2) represents the light source luminous intensity. Same formula (1-
C ₁ in 1) is C ₁ = I ₀ cosθ _e − Asinα _e + (B + Aα _e )
It is obtained by cosα _e . However, θ ₀ is the initial value of the angle θ, and α ₀ is the reflection angle at that time. Also (1-
2) C ₂ in the formula is obtained by C ₂ =−Icosθ _K +B. However, θ _K = cos ^-1 [{(AsinΔQ)-(B+A×
Δα) cosΔα+C ₁ }/I ₀ ]. When a lighting lamp is constructed using the reflector 4 constructed as described above, the reflected light arrow shown in FIG.
As shown in R _a , R _b , ~ _{R e} , the reflection angles α _a , α _b , ~ α _e become larger from the center toward the periphery. In this way, among the reflected light beams, those near the center (e.g., R _a ) intersect with the optical axis Z-Z, while the peripheral portions (e.g., R _e ) are diffused.
Therefore, even if the lens 5 is set large and the depth of the reflecting mirror 4 is set shallow, the efficiency of using the light emitted from the light source 2 is high. The reflected light beams R _a to _{R e} shown below the optical axis Z-Z in FIG. 7 provide a luminous intensity distribution as shown in FIG. By the reflected lights R _a ' to R _e ', a luminous intensity distribution as shown in FIG. 8C, which is symmetrical to FIG. 8B, is obtained. When FIG. 8B and FIG. 8C are superimposed, the result is as shown in FIG. 8D, where the shaded area is where the reflected lights from both overlap. When the algebraic sum of the light intensity curves for the above-mentioned overlapping portions is calculated graphically, it becomes as shown in FIG. 8A, and a desired light distribution pattern can be obtained. When a lamp having the light distribution characteristics shown in Fig. 8A is applied to a car stop light, for example, the maximum luminous intensity area in the center is much brighter than the surrounding area, so it will not attract the attention of following cars. can. By applying the above principle and setting |α _a =α _e |, the entire irradiation area can be illuminated almost uniformly. In actual problems, the luminous intensity distribution of the reflected light set as described above overlaps with the luminous intensity distribution of the light directly projected forward from the light source. Therefore, when implementing the present invention, it is desirable to take directly projected light into consideration during the step of setting the desired reflected light distribution characteristics. A specific example of a reflective mirror according to the present invention based on the above calculation will be described below with reference to FIG. FIG. 10 is a diagram for explaining the design calculation of the reflecting mirror of the present invention, where Z-Z is the coordinate axis that becomes the optical axis, and
-X is a coordinate axis perpendicular to the Z-Z axis, D is the radius of the mirror aperture, and F is the focal point. The illustrated section V is a portion that does not constitute a reflective surface because a hole for inserting a light source bulb is provided. Let the coordinates of the focal point F be (0, 0). This focus F
When a light source is placed at , the minimum value of the angle θ of the light incident on the reflective surface M with respect to the optical axis is θ ₀ and the maximum value is θ _eod . The reflection angle (the angle that reflected light makes with respect to the optical axis) when θ ₀ is α ₀ , and the reflection angle when θ _eod is α _eod . Light source luminous intensity I ₀ = 4 cd, target luminous intensity I ₀ = 25 cd in α ₀ direction,
α Target luminous intensity in the _eod direction I _eod = 17 cd, aperture radius D =
Within 110mm, α ₀ = −20°, α _eod = 40°, θ ₀ = 40°,
Set the values of (x ₀ , z ₀ ) to (14.559, −17.351).
Assuming that the distance f from the light source position to the apex of the reflective surface is 20 mm, calculations are performed using equations (1-1), (1-2), (2), and (3). In this example, we input the above conditions into a computer and calculated the values of (x, z) and θ at every 1° from α = -20° to α = 40°. . The results are shown in the table below.

【table】

[Table] Further, as an example different from the above, a calculation example is shown below in which settings are made to obtain substantially uniform luminous intensity throughout the irradiation range. In this example, I ₀ = 4cd,
θ ₀ = 40°, D = within 200mm, α ₀ = -20°, α _eod = 20°,
I ₀ = 60cd, I _eod = 35cd (x ₀ , z ₀ ) coordinate value = (14,
559, -17, 351), and was calculated by setting f = 20 mm.

[Table] In these embodiments, the light reflected by the reflecting mirror 4 (FIG. 7) has almost the desired light distribution pattern as described above, so that the necessity of light adjustment by the lens 5 is low. For this reason, the lens 5 is constructed of a transparent flat lens. Although it is not possible to prevent the use of a prism lens as a lens used together with the reflecting mirror of the present invention, even if a prism lens is used, there is no need to use a thick lens or a prism with a complicated shape. As described in detail above, according to the present invention, the light distribution characteristics can be set arbitrarily, and in particular, the luminous intensity at an arbitrary radius near the center can be made to be more than twice the luminous intensity at other parts. It is also possible to make the luminous intensity uniform over the entire illumination range, and even if the depth of the reflector is set shallow using a simple lens with a large area, the effective utilization rate of the light emitted from the light source can be reduced. This has an excellent practical effect in that it is possible to construct a reflecting mirror for a lamp with a large size.

[Brief explanation of drawings]

Figures 1 to 4 show an example of a conventional lighting lamp, with Figure 1 being a cross-sectional view, Figure 2 being a partial front view, and Figure 3 being a light distribution pattern when using a spherical prism. The chart, FIG. 4, is also a chart showing the luminous intensity distribution. FIG. 5 is a chart showing an example of a light distribution pattern when a semicylindrical prism is used in a conventional lighting lamp. 6 to 9 show one embodiment of the reflector for a lamp according to the present invention, FIG. 6 is an explanatory diagram of setting a curved surface, FIG. 7 is a cross-sectional view, and FIG. 8 is a diagram showing desired luminous intensity distribution characteristics. FIG. 9 is a chart showing the light distribution pattern. FIG. 10 is an explanatory chart of design calculations in an embodiment of the present invention. 1... conventional reflecting mirror, 2... light source, 3... lens, 3a... prism surface of lens, 4... reflecting mirror, 5... lens.

Claims (1)

[Scope of Claims] 1. In a reflecting mirror for reflecting a part of the luminous flux emitted from a light source of an illumination lamp toward the front, the light incident from the light source toward a reflecting surface with the position of the light source as a reference. The angle θ with respect to the optical axis of
The relationship between the luminous intensity I ₀ of the light source and the angle α of the reflected light with respect to the optical axis is set so that α > 0 at the center of the mirror surface, so that I ₀
cosθ=Asinα−(B+Aα)cosα+C ₁ , and at _the periphery of the mirror surface, α≧ _0. The coordinates (x ₁ , z ₁ ) of the point of incidence at angle θ and the coordinates (x ₂ , z ₂ ) of the point of incidence at angle θ + Δθ
_{The relationship between}
(θ−α/2) and z ₂ =−{x ₁ tan(θ−α/2)−z ₁ }/1+tan(θ+Δ
It has a continuous curved surface formed by rotating a continuous curve expressed by A reflector for a lamp, characterized in that the angle α is set to increase as the angle θ increases. However, the above A, B,
C ₁ and C ₂ are constants that can be selected from a design perspective to determine the light distribution characteristics of reflected light.