The present invention relates to a projection lens assembly and a related projection apparatus, and more particularly to a projection lens assembly and a related projection apparatus capable of spontaneously compensating the focus shift/defocus caused by thermal shift.
In order to save costs, the conventional projection apparatus usually use aspherical lenses as the projection lens. Basically, the aspherical lenses are made of plastic; thus, a poor production yield may occur if the projection apparatus has a relatively large number of aspherical lenses. In addition, with the increased brightness of projection apparatus, the plastic aspherical lenses may have some defects caused by heat, such as thermal shift and coating separation. Particularly, the heat the optical engine suffering increases with the operation time of the projection apparatus, which changes the refractive index of the optical elements in the optical engine and makes the metal casing of the optical engine expanded, and results in focus shift/defocus of the projection lens; thus, the thermal shift happens and the imaging quality is negatively affected. Therefore, it is quite important to design a projection lens assembly capable of compensating the thermal shift and avoiding the focus shift/defocus.
Therefore, one object of the present invention is to provide a projection lens assembly and a projection apparatus capable of spontaneously compensating the focus shift/defocus caused by thermal shift.
The present invention provides a projection lens assembly, which includes a first lens group and a second lens group. The first lens group has a negative dioptre and is disposed adjacent to an object side. The first lens group includes a first lens having a negative dioptre. The second lens group has a positive dioptre and is disposed adjacent to an image side. The second lens group includes a second lens having a positive dioptre and a third lens having a negative dioptre. The second lens is disposed between the first lens and the third lens. The third lens is made of heavy flint glass. A temperature coefficient of refractive index of the second lens represents D0, and −3.0×e−5≦D0≦−6.0×e−7.
The present invention further provides projection apparatus for projecting an image onto a screen. The projection apparatus includes a light source, an imaging unit and a projection lens assembly. The light source is for providing a light. The imaging unit is for receiving the light. The projection lens assembly is disposed between the imaging unit and the screen and for projecting the light onto the screen. The projection lens assembly includes a first lens group and a second lens group. The first lens group has a negative dioptre and is disposed adjacent to the screen. The first lens group includes a first lens having a negative dioptre. The second lens group has a positive dioptre and is disposed adjacent to the image side. The second lens group includes a second lens having a positive dioptre and a third lens having a negative dioptre. The second lens is disposed between the first lens and the third lens. The third lens is made of heavy flint glass. A temperature coefficient of refractive index of the second lens represents D0, and −3.0×e−5≦D0≦−6.0×e−7.
Summarily, in the present invention, all of the lenses in the first and second lens groups are spherical lenses, preferably. The third lens is made of heavy flint glass to eliminate the chromatic aberration of the projection lens assembly. The second lens is used to compensate the thermal shift of the third lens and the expansion of the optical engine, wherein temperature coefficient of refractive index (the varying ratio of the refractive index affected by temperature difference) of the second lens represents D0, and −3.0×e−5≦D0≦−6.0×e−7. Thus, compared with the conventional technology, the projection lens assembly and the related projection apparatus of the present invention have some specific advantages such as lower manufacturing cost and easier operation. In addition, the projection lens assembly and the related projection apparatus of the present invention can provide qualified thermal shift compensation effect in response to the high brightness projection demand.
For making the above and other purposes, features and benefits become more readily apparent to those ordinarily skilled in the art, the preferred embodiments and the detailed descriptions with accompanying drawings will be put forward in the following descriptions.
The present invention will become more readily apparent to those ordinarily skilled in the art after reviewing the following detailed description and accompanying drawings, in which:
The present invention will now be described more specifically with reference to the following embodiments. It is to be noted that the following descriptions of preferred embodiments of this invention are presented herein for purpose of illustration and description only. It is not intended to be exhaustive or to be limited to the precise form disclosed.
Please refer to
In one preferred embodiment, the third lens 32 is a biconcave (concave-concave) lens, and made of heavy flint glass. Because of having the properties of higher refractive index and higher dispersion coefficient, the heavy flint glass herein is mainly used for eliminating the chromatic aberration of the projection lens assembly 18. In response to the material properties of the heavy flint glass, preferably, the refractive index of the third lens 32 is between 1.64 and 1.87 and the Abbe number of the third lens 32 is between 20 and 35. In the present invention, the third lens 32 usually has a specific lens model such as S-TIH or S-TIM; however, the present invention is not limited thereto.
When the focusing of the projection apparatus 10 is completed, the third lens 32 may have a relatively large thermal shift due to having the metal casing of the projection apparatus 10 being expanded by heat increasing with the operation time; thus, the best focus may move to be in front (or, left) of the imaging unit 16 (equivalently, the back focal length is becoming longer) and the projection lens assembly 18 may have or experience focus shift/defocus. To compensate the aforementioned thermal shift, the second lens 30 is disposed between the first lens 28 and the third lens 32 in the present invention. Specifically, the temperature coefficient of refractive index of the second lens 30 is represented by D0 and the refractive index of the second lens 30 is represented by n, wherein −3.0×e−5≦D0≦−6.0×e−7 and n≧1.57. The temperature coefficient of refractive index herein is defined as the ratio of the variation of the refractive index to the temperature difference
(and is equivalent to
Specifically, the focus point has a smaller position change when the temperature coefficient of refractive index is higher than an upper limit. On the contrary, a smaller temperature coefficient of refractive index can result in a better compensation effect. In the present invention, the temperature coefficient of refractive index of the second lens 30 is represented by D0 and D0 is not smaller than −3.0×e−5 due to the limitation of the material properties of lenses. Table 1 lists several lens models applicable to the second lens 30 of the present invention.
Preferably, the thermal shift is compensated by the second lens 30 in the present invention. However, it is understood that more than one lens may be employed if the thermal shift compensation effect provided by the one single second lens 30 is not as expected. For example, in one embodiment, the second lens group 26 may selectively include a fourth lens 34 having a positive dioptre and a fifth lens 36, which are disposed on the two opposite sides of the third lens 32, respectively. The fourth lens 34 herein is used to enhance the compensation of the thermal shift of the projection apparatus 10. It is to be noted that the aforementioned amount/number and the dioptre characteristics of the lenses in the second lens group 26 are provided for an exemplary purpose only, and the present invention is not limited thereto. The second lens group 26 may be any combination of lenses which can provide lights polymerizable function, and the following will not describe the same or similar optical characteristics of other embodiments in detail. Table 2 lists preferred parameter values of each spherical lens of the projection lens assembly 18. In Table 2, “interval” represents the distance between the surfaces in the current row and in the next adjacent row.
Please refer to
As shown in
In the projection apparatus 10 of the present invention, the thermal shift is eliminated by employing the second lens 30 having a positive dioptre and/or the fourth lenses 34. That is, the thermal shift of the projection apparatus 10 is mainly eliminated by the second lens 30 and the fourth lens 34 is selectively utilized depending on actual thermal shift elimination effect provided by the second lens 30. As shown in
In one preferred embodiment, the projection lens assembly 18 is a non-telecentric system. Table 3 lists the preferred focal length of each optical component in the present invention. For example, the effective focal length f of the projection lens assembly 18 is 21.9 mm; the effective focal length f1 of the first lens 28 is −49.61 mm; and the effective focal length f3 of the third lens 32 is −13.343801 mm; wherein
are lower than a lower limit, then |f1| and |f3| are relatively small and the related lenses have a relatively high dioptre; as a result, the chromatic aberration issue may happen. In addition, if
are lower than a lower limit, then the projection lens assembly 18 needs more lenses and accordingly has a greater thermal shift which is not the issue the projection lens assembly 18 in the present invention applies for. On the contrary, if
are higher than an upper limit, then |f1| and |f3| are relatively large and the related lenses have a relatively low dioptre; as a result, the projection lens assembly 18 may have a relatively low magnification, which may not meet the needs or demand from user.
Summarily, in the present invention, all of the lenses in the first and second lens groups are spherical lenses, preferably. The third lens is made of heavy flint glass to eliminate the chromatic aberration of the projection lens assembly. The second lens is used to compensate the thermal shift of the third lens and the expansion of the optical engine, wherein temperature coefficient of refractive index (the ratio of the variation of the refractive index to the temperature difference) of the second lens is represented by D0, and −3.0×e−5≦D0≦−6.0×e−7. Thus, compared with the conventional technology, the projection lens assembly and the related projection apparatus of the present invention have some specific advantages such as lower manufacturing cost and easier operation. In addition, the projection lens assembly and the related projection apparatus of the present invention can provide qualified thermal shift compensation effect in response to the high brightness projection demand.
While the invention has been described in terms of what is presently considered to be the most practical and preferred embodiments, it is to be understood that the invention needs not be limited to the disclosed embodiment. On the contrary, it is intended to cover various modifications and similar arrangements included within the spirit and scope of the appended claims which are to be accorded with the broadest interpretation so as to encompass all such modifications and similar structures.
Number | Date | Country | Kind |
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103109737 | Mar 2014 | TW | national |