The invention is directed towards optical devices, and more specifically, towards optical conduits that efficiently capture light from a light source and redirect it onto a surface for illumination.
An optical mouse operates by scanning an illuminated surface with an optical sensor and acquiring a series of images of the surface. The optical mouse then determines its own position relative to the surface by comparing the differences between the images. The light source used for illuminating the surface is typically a light-emitting diode (LED). Since the light emitted by an LED is dispersed over a wide angle, an optical conduit is used to channel and focus the light from the LED onto the surface.
Since the efficiency of the prior art optical conduit 101 is poor, the power of the LED 103 needs to be increased to adequately illuminate the surface 105. Increasing the LED power is not a problem when the optical mouse is attached by a cord to a desktop computer system. However, power consumption is a big concern in applications such as laptops or battery-powered cordless mice. Therefore, a more efficient optical conduit is needed.
In a preferred embodiment of the present invention, an optical conduit for channeling light from a light source onto a surface is created by combining the optical conduit with the light source to create a single component. The optical conduit has an input end for light input, and an output end where the light exits the optical conduit to fall onto the surface. When the optical conduit is made of a moldable material, the light source can be embedded into the input end of the optical conduit itself. Alternatively, the light source can be glued to the exterior of the input end of the optical conduit.
In an alternate embodiment, the light source within the optical conduit is surrounded by a reflective cup. The reflective cup captures light rays that would otherwise escape the optical conduit because they were emitted in the wrong direction, and redirects them towards the output end of the optical conduit.
In an alternate embodiment, the optical conduit is in the shape of a paraboloid. The curved interior surface of the paraboloid is more efficient at collecting and concentrating light than a flat surface.
Further features and advantages of the present invention, as well as the structure and operation of preferred embodiments of the present invention, are described in detail below with reference to the accompanying exemplary drawings. In the drawings, like reference numbers indicate identical or functionally similar elements.
The refractive index n of the optical conduit 201 is higher than that of the surrounding medium, which is typically air. Possible choices of material for the optical conduit 201 include acrylic, polycarbonate, optical grade plastics, or any other material optically transmissive to light in the visible and infrared spectrum range.
A light source 209, such as an LED, is embedded directly in the optical conduit 201. More light is captured in this arrangement than in the prior art, since light rays emitted by the light source 209 now originate from within the optical conduit 201 itself. The optical conduit 201 is preferably made of a moldable material, so that the light source 209 may be inserted into the optical conduit before the material cures and sets. Any light rays, such as exemplary light ray 211, that hit the interior surface at an angle A1 greater than the critical angle θc will be totally internally reflected. θc is determined by Snell's law: sin θc>ns/n ; where ns is the index of refraction for the surrounding medium, and n is the index of refraction for the conduit itself.
The light 211 travels along the optical conduit 201, reflecting off the flat interior surface of the sidewalls 203 towards the output end 207. The light 211 hits each wall at an angle greater than the critical angle and is reflected back into the optical conduit 201. The light 211 finally exits through the output end 207 to strike the surface to be illuminated. Since the light source 209 and the optical conduit 201 are now one piece, there is no loss of light due to separation between the light source 209 and the optical conduit 201. In an alternate embodiment (not shown), the light source 209 is glued directly to the exterior surface of the optical conduit 201 at its input end 205, using optically transmissive glue.
Since the light source 209 radiates light in all directions, many of its light rays are radiated in a direction away from the output end 207 such that the light rays escape the optical conduit 201 without being totally internally reflected towards the output end 207. By surrounding the light source 209 with a reflective surface to capture and redirect such light rays, the efficiency of the optical conduit 201 can be further increased.
The paraboloid 301 has an input end 305 for light input, and an output end 307 for light output. A light source 209 surrounded by a reflector cup 213 is embedded into the input end 305, such that the opening of the reflector cup 213 is facing the output end 307. In an actual working embodiment, a paraboloid having an embedded light source surrounded by a reflector cup achieved efficiencies around 16%, which is a 60% increase over the old efficiency.
sin A3≦1−(2/n2), (Equation 1)
or
sin A4≦n−(2/n), (Equation 2)
where n is the index of refraction for the paraboloid 301.
In general, a curved surface is more efficient at collecting and concentrating light rays than a flat surface. Therefore, an optical conduit with a curved surface will be more efficient than a flat-sided optical conduit. Other suitable surfaces have curvatures fitting parabolic equations, hyperbolic equations, or any equations of second-order or higher, as long as the surface curvatures still satisfy equation 1 or 2. For example, an optical conduit in the shape of a hyperboloid (a solid of revolution formed by rotating a hyperbola around its axis of symmetry) will have improved performance over a flat-sided optical conduit.
A combination of different curvatures may also be used. For example, in
To facilitate the illumination of a surface, a gradual bend may be introduced between the input and output ends of the optical conduit, after the proper surface curvature for the optical conduit has been determined by equation 1 or 2.
Although the present invention has been described in detail with reference to particular preferred embodiments, persons possessing ordinary skill in the art to which this invention pertains will appreciate that various modifications and enhancements may be made without departing from the spirit and scope of the claims that follow.