JP2004029685A - Method and device for fixed magnification imaging using variable focal lens - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To obtain a method and a device for variable focal imaging which form an image of an object in a fixed position by focusing and allow focusing with a fixed imaging magnification . <P>SOLUTION: An imaging optical system is constituted of a convergent lens 2 and a variable focal lens 4 changing the focal length which are arranged such that an object principal point of the vari-focal lens 4 coincides with an image focus of the convergent lens 2, and the focal length of the variable focal lens 4 is adjusted so as to form an image 5 of an object 1 in the fixed position, and the object is focused on. <P>COPYRIGHT: (C)2004,JPO

Description

[0001]
BACKGROUND OF THE INVENTION
The present invention is used in the field of image applications such as various monitoring systems, traffic measurement systems, autonomous vehicles, and devices for automatically inspecting the appearance of products. The present invention relates to a method and apparatus for obtaining an image in focus.
[0002]
[Prior art]
As a method of focusing, a method of moving a lens back and forth according to the position of an object has been common so far as seen in a general camera. However, in recent years, a transparent liquid is sandwiched between glass circular thin plates to form a structure with a lens action, and this lens structure is subjected to pressure by a piezo actuator to change the curvature of the glass surface. A variable focus lens that can change the speed at high speed has been realized. Then, using such an electrically controllable variable focus lens in combination with an objective lens of an observation microscope, the focal length is changed at high speed during the afterimage time of the eye, and each part of a deep object is sequentially and rapidly Research has been reported to achieve a 3D product visual inspection system with a deep depth of focus by focusing (Takane Kaneko, Nobuyuki Ohya, Nobuaki Kawahara, Long-Focus-Depth Vision System using Variable-Focus Lens, DENSO) Technical Review, Vol. 3, No. 1, pages 52 to 58, 1998). In addition, a lens structure suitable for high-speed control using a multilayer piezo actuator has been designed, and production examples of high-speed variable focus lenses that can change the focal length at a period of 1 kHz have been reported (Oku Hiromasa, Ishikawa Masatoshi, kHz Prototype of a variable focus lens that can respond on the order, Proceedings of the Japan Society of Mechanical Engineers No. 02-6 Robotics and Mechatronics Lecture, 2P2-J09 (1)-(2), June 2002). On the other hand, a focusing method using a variable focus mirror that can change the focal length by controlling the curvature of the mirror surface by an external force such as fluid pressure or electrostatic force instead of a lens has been devised (see FIG. Published Patent Publication: JP-A-2002-122779). By installing the variable focus mirror at the image focal point of the focusing lens for imaging, it is possible to focus on different object positions while keeping the imaging magnification constant.
[0003]
[Problems to be solved by the invention]
The above conventional techniques have the following problems. First, in the method of focusing by moving the lens, since the mass of the lens is large, it is difficult to perform high-speed repeated focusing operation of about 30 to 60 Hz, which is comparable to the update period of the TV camera image or the afterimage time of the eye.
[0004]
In the focusing method using the variable focus lens, the focal length of the lens changes, so that the focus can be adjusted, but the imaging magnification also changes, and the size of the image changes. For this reason, in the field of measuring dimensions and shapes, it is necessary to correct the size of the obtained image data, and it takes a lot of time for computer processing of the image data, which is disadvantageous for speeding up.
[0005]
In the focusing method using a variable focus mirror, an optical device such as a semi-transparent mirror or a polarizing beam splitter is used to separate the incident light to the focusing optical system and the focused outgoing light reflected by the mirror. Since separation means is required, there is a drawback that the entire optical system becomes complicated.
[0006]
The present invention has been made under such circumstances, and for a solid body having a depth, the imaging magnification is kept constant at a high speed similar to the image acquisition speed in the television system. An object of the present invention is to realize a simple focusing method capable of focusing on each part of a solid in a state.
[0007]
[Means for Solving the Problems]
In order to solve the above-described problem, in the present invention, the light generated from each point of the object with respect to an object arranged at an arbitrary distance from the focal point is referred to as an object focal point (also referred to as a front focal point) of the converging lens. The light is incident on the converging lens, and light emitted from the converging lens is incident on a variable focus lens installed at an image focal point (also referred to as a rear focal point) of the converging lens. Then, by setting the focal length of the variable focus lens according to the distance of the object position to be focused, the object image is formed at a constant position at a constant magnification regardless of the position of the object to be focused. It is a thing.
[0008]
DETAILED DESCRIPTION OF THE INVENTION
Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the drawings.
[0009]
FIG. 1 is a schematic representation of a cross-sectional view of an imaging optical system in order to show the configuration of a method and apparatus for obtaining an object image by focusing at a constant magnification according to the present invention. 1 is an object to be focused, 2 is a convergent lens, 3 is an image of the object 1 generated by the convergent lens 2, 4 is a variable focus lens, and 5 is an image of an object obtained by the convergent lens 2 and the variable focus lens 4. is there. Reference numeral 6 denotes an optical axis serving as a central axis of the optical system. F1 and F2 are an object focal point (sometimes referred to as a front focal point) and an image focal point (also referred to as a rear focal point), respectively. S indicates the position of the object image 5 on the optical axis. If the focal length of the varifocal lens 4 is signed and takes a positive value for a convex lens and a negative value for a concave lens, the same lens imaging formula can be applied to both convex and concave lenses.
[0010]
When the object 1 is located at a distance p from the object focal point F1 in the object space (also referred to as an object space) of the converging lens 2, the image 3 is generated at a distance q from the image focal point F2 of the converging lens 2. The distance relationship is given as f / p = q / f by the lens imaging formula, where f is the focal length of the convergent lens 2. Here, the symbol / represents division. Further, p> 0 indicates that the focusing position is forward from the object focal point F1 (a direction away from the converging lens 2), and p <0 is backward from the object focal point F1. The light forming the object image 3 is re-imaged by the variable focus lens 4 to finally form the object image 5. Here, the focal length of the varifocal lens 4 is fc, the object principal point (also referred to as the front principal point) not shown in the figure of the variable focus lens 4, and the image principal point not shown in the figure of the convergent lens 2. Is the distance between the image and the optical path length from the image principal point (also referred to as the rear principal point) not shown in the figure of the variable focus lens 4 to the position S of the object image 5, s. The optical path length s that determines the position S is given as a value satisfying the equation 1 / (df−q) + 1 / s = 1 / fc from the lens imaging formula. Therefore, by setting the focal length fc of the variable focus lens 4 so as to satisfy the above equation according to the position p (= f × f / q) of the focusing surface of the object so that the optical path length s becomes constant, An object image can be formed at the fixed position S. At this time, the imaging magnification m is calculated from the product of the imaging magnification (−f) / p of the converging lens 2 and the imaging magnification (−s) / (df−q) of the variable focus lens 4. s / f) / {1- (df) / q}. Here, when d = f, that is, by making the object principal point of the variable focus lens 4 coincide with the image focus F2 of the converging lens 2, the imaging magnification m is related to the object position p (= f × f / q). Instead, it can be a constant value (−s) / f. A negative sign indicates an inverted image. Actually, the allowable setting error when the object principal point of the variable focus lens 4 and the image focus of the converging lens 2 are matched is determined by the limit value of the allowable variation amount of the imaging magnification m. In the present invention, matching means matching within a tolerance range. When the variable focal length lens 4 changes the focal length fc, the principal point position generally changes, but if the fluctuation of the principal point position is sufficiently smaller than the focal length f of the converging lens 2, the fluctuation of the magnification is practical. Can be ignored. When the object principal point of the varifocal lens 4 and the image focus of the converging lens 2 coincide with each other under the condition of a constant magnification and d = f, the focal length fc of the varifocal lens 4 is q × s for focusing. / (Q-s) or f / {(f / s)-(p / f)}. Here, when the relationship of p × s <f × f is established, the focal length fc is a positive value, so the variable focus lens 4 is a convex lens (generally a converging lens), and p × s> f × f. When the relationship is established, the focal length fc is a negative value, so the variable focus lens 4 is a concave lens (generally a diverging lens), and the focal length fc is infinite if p × s = f × f. Therefore, the variable focus lens 4 is an optical medium equivalent to a plane parallel plate having no refractive power.
[0011]
In the embodiment of the invention shown in FIG. 1, the object image 5 is generated at a position separated from the image principal point of the varifocal lens 4 by a finite optical path length s. As a second embodiment, an embodiment in which an object image by the converging lens 2 and the variable focus lens 4 is generated at infinity will be described with reference to FIG. The relational expression giving the relationship between the imaging distance s and the focal length fc of the variable focus lens 4, where the imaging distance s is infinite, and the image principal point of the variable focus lens 4 is at the image focal position of the converging lens 2. When d = f, the value of the focal length fc necessary to generate an object image by the converging lens 2 and the variable focus lens 4 at infinity is −q or −f × f / p. At this time, if the position of the object to be focused is in front of the object focus of the convergent lens 2, if p> 0, the focal length fc takes a negative value, and the variable focus lens 4 is a concave lens (divergent lens). . On the other hand, if the position of the object to be focused is behind the object focus of the convergent lens 2, p <0, so the focal length fc takes a positive value, and the variable focus lens 4 is a convex lens (convergent lens). When p = 0, that is, when the focusing position is on the object focal plane of the converging lens 2, the focal length fc is set to infinity, and the variable focus lens 4 is an optical medium equivalent to a parallel flat plate having no refractive power. Set to. The embodiment shown in FIG. 2 shows a case where p> 0. The difference from the embodiment shown in FIG. 1 is that it is necessary to re-image within a finite distance in order to use the image of an object at infinity, and a focusing lens 7 is added to the focal plane. An object image 51 is obtained. Regardless of the position p of the object, if the image formed at infinity by the convergent lens 2 and the variable focus lens 4 is re-imaged at the position of the focal plane of the convergent lens 7, and the focal length of the convergent lens 7 is fr, The imaging magnification m is a constant value as a focal length ratio (−fr) / f.
[0012]
In the first embodiment, if the reference distance is p = f × f / s, and in the second embodiment, the reference distance is p = 0, the focal length of the variable focus lens necessary for focusing is set to infinity. That is, focusing can be performed by increasing / decreasing the refractive power from zero, and the configuration of the variable focus lens becomes easy. In particular, in a variable focus lens that changes the focal length by changing the curvature of the lens surface, it is only necessary to change the lens surface from a flat surface to a slightly spherical surface, which is a preferable operating condition.
[0013]
In the above-described embodiment, the specific configuration of the variable focus lens 4 capable of adjusting the focal length has not been described so far, but can be realized by various configurations. As an example of the embodiment, a configuration similar to that cited when referring to the prior art, such as a cross-sectional view in FIG. 3 and a front view in FIG. 4, can be considered. Two opposing circular openings 10 of a lens container 9 filled and sealed with a transparent liquid 8 such as silicone oil are each covered with a glass thin plate 11, and the glass thin plate 11 is fixed around the circular opening 10. Construct a structure. Reference numeral 12 denotes an optical axis of a lens passing through the center of the circular opening 10. Reference numeral 13 denotes an elastic plate made of metal or glass, which is pressurized by the laminated piezoelectric actuator 14 and controls the internal pressure of the sealed transparent liquid 8. The glass thin plate 11 is elastically deformed into a spherical shape by the differential pressure between the internal pressure and the atmospheric pressure, and forms a convex lens if it is positive pressure and a concave lens if it is negative pressure, and various focal length values depending on the degree of deformation. Is realized. If the differential pressure is zero, it becomes a transparent parallel plate with an infinite focal length. Reference numeral 15 denotes a voltage amplifier for applying a voltage necessary for the deformation of the thin glass plate 11 to the laminated piezoelectric actuator 14. Reference numeral 16 denotes a voltage signal sent to the voltage amplifier 15 to control the focal length of the variable focus lens by the deformation of the thin glass plate 11. It is a controller to do.
[0014]
Another embodiment of the variable focus lens 4 is shown in FIG. Reference numerals 17 and 18 denote a convex lens and a concave lens, which are equal in size and have opposite focal lengths, and are arranged with the optical axis 19 matched and spaced apart by a distance g to constitute a variable focus lens as one combination lens. Yes. The focal length fc of this variable focal length lens is fo × fo / g, where fo is the focal length of both lenses. However, the interval g is a distance between the rear principal point of the convex lens 17 and the front principal point of the concave lens 18, and takes a positive sign when the rear principal point of the convex lens is in front of the front principal point of the concave lens, In the opposite case, it takes a negative sign. When g = 0, the focal length is infinite, and the focal length can be greatly increased / decreased by slightly increasing / decreasing the distance between the light-weight concave and convex lenses. Adjustment is possible. Although not shown, the distance g can be adjusted by moving one or both lenses along a linear trajectory using a piezo actuator or a voice coil actuator, and can be easily realized by conventional techniques. In the description of the above embodiment, the focal lengths of the convex lens and the concave lens are the same. However, even if they are slightly different, if the gap g is adjusted by increasing / decreasing the gap g by an amount corresponding to the size difference, Can have the same effect. Moreover, even if both the convex lens and the concave lens are configured by combining a plurality of lenses, the same functional effect can be obtained. However, if there is no problem in terms of lens aberration correction, the use of a single lens can minimize the mass, which is advantageous for controlling the gap g by high-speed movement of the lens. The chromatic aberration can be reduced by selecting and combining the materials of the convex lens and the concave lens.
[0015]
Compared with the variable focus lens described with reference to FIGS. 3 and 4 which is filled with a transparent liquid and does not have a lens structure and controls deformation of the lens when used, the variable focus for controlling the gap between the concave and convex lenses described in FIG. Since the lens surface shape can be precisely prepared in advance by a precision processing technique, the lens is advantageous in realizing a high-quality variable focus lens with little aberration.
[0016]
Since the refractive index of the liquid crystal can be changed by applying a voltage, this characteristic can be used to add a voltage distribution to the liquid crystal panel to create a refractive index distribution, thereby exhibiting a lens function. At present, there is a drawback that the response speed is slow and the transmission wavelength range is limited. one of.
[0017]
In the above description of the embodiment, the object is an object, but it is optically clear that the present invention can be applied to an optical image formed by another optical device.
In this case, the optical image generated in the object space of the converging lens 2 is re-imaged by the converging lens 2 and the variable focus lens 4, and the re-imaging magnification is constant regardless of the focus position of the optical image.
[0018]
In the description of the embodiment, the converging lens 2 is generally a compound lens composed of a combination of a plurality of lenses, and has a positive focal length similar to that of a single converging lens as a whole. It may be a more complex complex convergent lens system composed of a plurality of lenses and mirrors. At this time, the object principal point of the varifocal lens 4 is set at the image focal point of the compound lens system in the same manner as described in the above embodiment, and the combined focal length of the compound lens system is that of the convergent lens 2. Treated as focal length f.
[0019]
【The invention's effect】
The present invention has the following effects when implemented in the form as described above.
[0020]
Focusing is performed by making the object principal point of the variable focus lens coincide with the image focal point of the converging lens. Therefore, by controlling the focal length of the variable focus lens, the focal point can be set at an arbitrary position of the object to be obtained. And an image of the object can be obtained at a constant magnification.
[0021]
Therefore, as an application system of the present invention, in an image measurement system that receives an image of a focused object with a CCD camera and performs computer processing on the image information to perform object shape measurement and shape defect inspection, an image based on the position of the object Therefore, it is possible to measure the shape of the object at high speed and efficiently. In addition, since it is possible to avoid the occurrence of correction errors due to magnification correction, highly accurate shape measurement can be performed.
[0022]
What is required for a varifocal lens is that the focal length changes from infinity to a finite value, so only a slight structural change is required, and no large deformation of the curvature is required. It is easy to realize a quality variable focus lens. In particular, the operation speed can be increased in focusing based on the movement of the lens.
[0023]
Since transmitted light is used, the entire optical system is simplified as compared with a focusing method using a variable focus mirror that uses reflected light that requires a means for separating input and output light.
[0024]
In addition, when applying the present invention to an image of another optical device such as a telephoto lens, the re-imaging magnification is constant, and the shape of the image is not distorted. According to the present invention, there is provided a constant magnification variable focus imaging method and apparatus useful not only in the manufacturing field but also in image application systems in many fields of industry such as traffic measurement and facility monitoring. be able to.
[Brief description of the drawings]
FIG. 1 is a schematic cross-sectional view showing an embodiment of an optical system of a constant magnification variable focus imaging method and apparatus according to the present invention.
FIG. 2 is a schematic cross-sectional view showing another embodiment in which an image formed by a converging lens and a variable focus lens is formed at infinity in the optical system of the constant magnification variable focus imaging method and apparatus according to the present invention. is there.
FIG. 3 is a cross-sectional view showing an embodiment of a variable focus lens using a transparent liquid as a lens medium.
FIG. 4 is a front view of a lens opening showing an embodiment of a variable focus lens using a transparent liquid as a lens medium.
FIG. 5 is a cross-sectional view showing an embodiment of a variable focus lens that includes a convex lens and a concave lens and controls the gap between the two lenses.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 Object 2 to be focused 2 Converging lens 3 Image 4 of object 1 generated by converging lens 2 Variable focus lens 5 capable of changing focal length Image 6 of object obtained by converging lens 2 and variable focus lens 4 Optical system Optical axis 7 Converging lens 8 Transparent liquid 9 Lens container 10 Circular opening 11 Glass thin plate 12 Lens optical axis 13 Elastic plate 14 Laminated piezo actuator 15 Voltage amplifier 16 Controller 17 Convex lens 18 Concave lens 19 Optical axis

Claims (3)

An imaging method in which an object image is formed at a fixed position by focusing and an object image obtained by an object or other optical means is placed in the object space of a converging lens, and a variable focus lens is placed on the object The object is imaged at a constant magnification by arranging the point so as to coincide with the image focal point of the converging lens and changing the focal length of the variable focal lens to focus on the object or the object image. Alternatively, the constant-magnification variable-focus imaging method, wherein the object image is re-imaged. An imaging device that performs focusing and forms an image of an object at a fixed position, and includes a converging lens and a variable focal lens arranged so that the object principal point coincides with the image focal point of the converging lens. A constant-magnification variable-focus imaging device characterized in that focusing is performed at a constant magnification by changing a focal length of a focusing lens. The variable focus lens is configured as a combination lens composed of a convex lens and a concave lens having a close focal length, and the focal length of the variable focus lens is set by adjusting the distance between principal points of the convex lens and the concave lens. The constant magnification variable focus imaging method according to claim 1.

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