The present invention relates to a device for electrically controlling shaping of a light beam.
In many optical applications, it is desirable to control shape and direction of light originating from a light source, such as a light emitting diode (LED). In many applications, it is desirable to be able to control the shape of the light beam. Typically, a spot light that uses a reflector has a divergence of about 10° full-width half-maximum (FWHM) and flood light divergence is about 40° FWHM. In this context, the FWHM parameter is defined as the divergence angle at half the maximum intensity. In prior art, electrically switchable optical components such as lens arrays have been proposed to actively control the shape of a light beam. These types of components are, however, based on replication techniques that are expensive to implement in optical devices and systems. Moreover, most such components typically use cells where the liquid crystal molecules are uniaxially oriented parallel to the cell surface. In such a cell, application of an electric field alters only one of the polarization directions and thus only 50% of unpolarised light. In order to influence the other polarization direction, a second cell must be used. Disadvantageously, this results in significant additional losses of emitted light.
Electrically controlled scattering of light can be accomplished in many different ways. A common approach for accomplishing electrically controlled light scattering is to utilize polymer dispersed liquid crystals (PDLCs) or liquid crystal gels. PDLCs are created by means of dispersing liquid crystal molecules in an isotropic polymer. Typically, liquid crystal material is arranged between two glass plates with transparent electrodes, whereby a cell is formed. When no electric field is applied between the glass plates, the liquid crystals are randomly oriented which creates a scattering mode, wherein light is scattered in many directions. By applying an electric field, the scattering gradually decreases, and when the liquid crystals align parallel to the electric field, the crystal molecule refractive index match the polymer refractive index, wherein a transparent mode is created and light passes through the cell. LC gels on the other hand are created by dispersing liquid crystals in an oriented anisotropic polymer matrix. For LC gels with a negative dielectric anisotropy, the transparent mode is present when no electric field is applied. In the absence of an electric field, liquid crystal molecules are oriented in a direction perpendicular to the cell surfaces and consequently, there are no large-scale refractive index fluctuations within the LC cell. When an electric field is applied, the liquid crystals tend to become oriented perpendicular to the electric field and refractive index fluctuations are induced within the LC cell, and thus the scattering mode is activated.
European patent application having publication number 0 578 827 discloses an illuminator provided with a light source, a liquid crystal light regulating plate for scattering a desired amount of light emitted from the light source, and a control power source for controlling the light scattering rate of the liquid crystal plate. A part of the light emitted from the light source, which passes through the liquid crystal light regulating plate without being scattered, is utilized for illumination. By changing a control power source voltage applied for controlling the light scattering rate, it is possible to continuously change brightness of the illuminating light.
A problem in the publication 0 578 827 is that the liquid crystal light regulating plate scatters light to very large angles when operating in the particular voltage state that attains the scattering effect. When such an illuminator illuminates an object, a part of the light beam of the illuminator will not be incident on or adjacent to the object, but will be scattered to very large angles, away from the object. As a consequence, the regulating plate causes a light dimming effect.
An object of the present invention is to overcome the above-described problems and provide a device that enables electrically controlled shaping of light beams.
This object is attained by a device for electrically controlling shaping of a light beam according to claim 1.
In a first aspect of the present invention, there is provided a device comprising primary optics arranged to shape the light beam, an electrically controllable optical element arranged to alter the shaped light beam when in a light redirecting mode, and secondary optics arranged to shape the light beam altered by the electrically controllable optical element.
A basic idea of the present invention is to provide a device that enables electrically controlled shaping of a light beam. The device comprises primary optics that is arranged to shape the light beam. The light beam typically originates from a light source such as a LED, a laser or some other appropriate light source. The device further comprises an electrically controllable optical element arranged to change the direction of the light falling onto it when the element is in a light-redirecting mode. The optical element can be an electrically controllable scattering element e.g. created by using a PDLC material or liquid crystal (LC) gel. It can alternatively be a diffractive or refractive element. The degree of diffraction or scattering of the optical element is controlled by applying an electric field to the liquid crystal material, whereby the degree of scattering, diffraction or refraction varies with the applied electric field. Hence, in the light-redirecting mode, the optical element can e.g. scatter, diffract or refract the light impinging on it. Finally, the device comprises secondary optics arranged to shape the scattered, diffracted or refracted light beam from the optical element.
The present invention is advantageous, since it provides a polarization independent scattering effect, which can be realized using a single cell configuration. The optical element partially shifts the virtual position of the light source to a position at the optical element. Hence, the primary optics has the LED as the effective light source, while the secondary optics has the scattering element as the effective light source. Depending on the voltage that is applied to the optical element, the angular intensity pattern of the scattered, diffracted or refracted beam (i.e. the beam intensity versus beam divergence) can be varied.
According to an embodiment of the present invention, the primary optics is arranged to provide maximum light extraction as well as collimation for the part of the beam originating from the light source, the electrically controllable optical element is arranged to scatter the beam when in a scattering mode, and the secondary optics is arranged to shape light falling onto it to have a wider angular distribution. The secondary optics is further arranged to shape the non-scattered beam originating from the light source, which is not shaped by the primary optics when the electrically controllable optical element is arranged in a transparent mode. This embodiment is advantageous, since the total size of the primary and secondary optics becomes rather small when both the primary optics and the secondary optics are employed to shape the beam originating from the light source.
Further features of, and advantages with, the present invention will become apparent when studying the appended claims and the following description. Those skilled in the art realize that different features of the present invention can be combined to create embodiments other than those described in the following.
Preferred embodiments of the present invention will be described in more detail with reference made to the accompanying drawings, in which:
The LC gel material has the advantage that the cell will be in its transparent mode when the power is off, which in some applications might be preferred. For the choice of PDLC material versus LC gel material, one has to take into account the actual application.
a illustrates the device 200 when no electric field is applied to the transparent LC gel element 203, and
In
As can be seen from
Further, arrangements are possible in which multiple electrically controllable optical elements can be used in combination with other optical stages. In other words, multiple scattering elements and reflectors can be used in shaping the beam originating from a light source. Hence, a man skilled in the art realizes that a plurality of electrically controllable optical elements may be arranged in combination with static beam shaping elements.
Even though the invention has been described with reference to specific exemplifying embodiments thereof, many different alterations, modifications and the like will become apparent for those skilled in the art. The described embodiments are therefore not intended to limit the scope of the invention, as defined by the appended claims.
Number | Date | Country | Kind |
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04105104.6 | Oct 2004 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IB05/53321 | 10/10/2005 | WO | 00 | 4/11/2007 |