CN212515188U - Optical imaging lens - Google Patents

Optical imaging lens Download PDF

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Publication number
CN212515188U
CN212515188U CN202021666841.3U CN202021666841U CN212515188U CN 212515188 U CN212515188 U CN 212515188U CN 202021666841 U CN202021666841 U CN 202021666841U CN 212515188 U CN212515188 U CN 212515188U
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lens
optical
optical imaging
satisfy
image
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耿晓婷
戴付建
赵烈烽
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Zhejiang Sunny Optical Technology Co Ltd
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Zhejiang Sunny Optical Technology Co Ltd
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Abstract

The utility model discloses an optical imaging lens, it includes according to the preface by thing side to picture side along the optical axis: a first lens having a positive optical power; a second lens having a negative optical power; a third lens; a fourth lens having a positive optical power; a fifth lens element having a negative refractive power, the object-side surface of which is concave; the effective focal length f of the optical imaging lens, the entrance pupil diameter EPD of the optical imaging lens, the on-axis distance TTL from the object side surface of the first lens to the imaging surface, and the half of the diagonal length ImgH of the effective pixel area on the imaging surface can satisfy the following conditions: f/EPD <1.9 and TTL/ImgH < 1.25. The utility model discloses a control each lens's relevant parameter, provide an optical imaging system with big image plane, big light ring of becoming.

Description

Optical imaging lens
Technical Field
The utility model relates to an optical element technical field, in particular to optical imaging lens.
Background
In recent years, the ultra-thin mobile phone has been a market trend, the module technology is also continuously upgraded, wherein the requirement for the imaging quality of the mobile phone lens becomes higher and higher, under the situation, the more mobile phone lens lenses are made, the price also rises, for some manufacturers, the main trend is required to be followed to make the mobile phone lens with large image height, large aperture and ultra-thin, and higher cost performance is required.
The novel large-aperture back lens is 5 ultrathin large-aperture back lenses, has a larger imaging image surface, has ultrahigh cost performance, can provide a larger aperture, has unusual imaging quality even in a dark environment, becomes a flat replacement version of 6 lenses and 7 lenses, and can provide enough space for subsequent related adjustment due to the unique lens model, so that the related structure and the assembling process are more flexible.
SUMMERY OF THE UTILITY MODEL
Therefore, an optical imaging lens with five lenses is needed, is a five-lens ultrathin rear lens with large aperture, has a large imaging image surface, is ultrahigh in cost performance, can provide a large aperture, enables the imaging quality to be bad even in a dark environment, and becomes a flat replacement of six lenses and seven lenses.
The utility model provides an optical imaging lens, it includes according to the preface by thing side to picture side along the optical axis: a first lens having a positive optical power; a second lens having a negative optical power; a third lens having optical power; a fourth lens having a positive optical power; a fifth lens element having a negative refractive power, the object-side surface of which is concave; the effective focal length f of the optical imaging lens, the entrance pupil diameter EPD of the optical imaging lens, the on-axis distance TTL from the object side surface of the first lens to the imaging surface, and the half of the diagonal length ImgH of the effective pixel area on the imaging surface can satisfy the following conditions: f/EPD <1.9 and TTL/ImgH < 1.25.
In some embodiments, the effective focal length f1 of the first lens, the effective focal length f4 of the fourth lens, and the effective focal length of the optical imaging lens may satisfy: 1.7< (f1+ f4)/f < 2.2.
In some embodiments, an effective focal length f2 of the second lens and an effective focal length f5 of the fifth lens may satisfy: 2.4< f2/f5< 4.2.
In some embodiments, a radius of curvature R3 of the second lens object side surface and a radius of curvature R4 of the second lens image side surface may satisfy: 2.0< (R3+ R4)/(R3-R4) < 2.6.
In some embodiments, a radius of curvature R2 of the first lens image-side surface and a radius of curvature R1 of the first lens object-side surface may satisfy: 0.6< (R2-R1)/(R2+ R1) < 0.9.
In some embodiments, a center thickness CT1 of the first lens on the optical axis, a center thickness CT2 of the second lens on the optical axis, and a center thickness CT3 of the third lens on the optical axis may satisfy: 0.5< CT1/(CT2+ CT3) < 0.9.
In some embodiments, an air interval T34 of the third and fourth lenses on the optical axis, an air interval T12 of the first and second lenses on the optical axis, and an air interval T23 of the second and third lenses on the optical axis may satisfy: 1.5< T34/(T12+ T23) < 2.1.
In some embodiments, the effective focal length f of the optical imaging lens and the maximum field angle FOV of the optical imaging lens may satisfy: 3.1mm < f × tan (1/2FOV) <3.7 mm.
In some embodiments, a combined focal length f12 of the first lens and the second lens and an effective focal length f of the optical imaging lens satisfy: 1.2< f12/f < 1.7.
In some embodiments, between an edge thickness ET5 of the fifth lens and a center thickness CT5 of the fifth lens on an optical axis may satisfy: 1.4< ET5/CT5< 2.3.
In some embodiments, a center thickness CT4 of the fourth lens on an optical axis and an edge thickness ET4 of the fourth lens may satisfy: 1.2< CT4/ET4< 1.8.
In some embodiments, an on-axis distance SAG52 between an intersection of the fifth lens image-side surface and the optical axis to an effective radius vertex of the fifth lens image-side surface and an on-axis distance SAG51 between an intersection of the fifth lens object-side surface and the optical axis to an effective radius vertex of the fifth lens object-side surface may satisfy: 0.2< SAG52/SAG51< 0.7.
In some embodiments, the effective half aperture DT32 of the image side surface of the third lens and the effective half aperture DT22 of the image side surface of the second lens satisfy: 1.2< DT32/DT22< 1.5.
An optical imaging lens, an effective focal length f2 of the second lens and an effective focal length f5 of the fifth lens satisfying: 2.4< f2/f5< 4.2; and an air interval T34 of the third lens and the fourth lens on an optical axis, an air interval T12 of the first lens and the second lens on the optical axis, and an air interval T23 of the second lens and the third lens on the optical axis satisfy: 1.5< T34/(T12+ T23) < 2.1.
The optical imaging lens comprises five lenses, the focal power, the surface type and the center thickness of each lens and the on-axis distance between the lenses are reasonably distributed, and parameters such as the total optical length of the optical imaging lens are at least controlled, so that the optical imaging lens has at least one beneficial effect of large aperture, large image plane, large field angle, ultrathin performance and the like. The optical imaging lens is suitable for being used as a rear camera of portable electronic equipment such as a mobile phone.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings needed to be used in the description of the embodiments or the prior art will be briefly described below, it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to the structures shown in the drawings without creative efforts.
Fig. 1 is a schematic structural diagram of an optical imaging lens according to a first embodiment of the present invention;
fig. 2-5 show an axial chromatic aberration curve, an astigmatic curve, a distortion curve, and a magnification chromatic aberration curve of an optical imaging lens according to a first embodiment of the present invention;
fig. 6 is a schematic structural diagram of an optical imaging lens according to a second embodiment of the present invention;
fig. 7-10 show an axial chromatic aberration curve, an astigmatic curve, a distortion curve, and a magnification chromatic aberration curve of an optical imaging lens according to a second embodiment of the present invention;
fig. 11 is a schematic structural diagram of an optical imaging lens according to a third embodiment of the present invention;
fig. 12-15 show an axial chromatic aberration curve, an astigmatic curve, a distortion curve, and a magnification chromatic aberration curve of an optical imaging lens according to a third embodiment of the present invention;
fig. 16 is a schematic structural diagram of an optical imaging lens according to a fourth embodiment of the present invention;
fig. 17-20 show an axial chromatic aberration curve, an astigmatic curve, a distortion curve, and a magnification chromatic aberration curve of an optical imaging lens according to a fourth embodiment of the present invention;
fig. 21 is a schematic structural diagram of an optical imaging lens according to a fifth embodiment of the present invention;
fig. 22 to 25 show an axial chromatic aberration curve, an astigmatism curve, a distortion curve, and a magnification chromatic aberration curve of an optical imaging lens according to a fifth embodiment of the present invention.
The objects, features and advantages of the present invention will be further described with reference to the accompanying drawings.
Detailed Description
For a better understanding of the present application, various aspects of the present application will be described in more detail with reference to the accompanying drawings. It should be understood that the detailed description is merely illustrative of exemplary embodiments of the present application and does not limit the scope of the present application in any way. Like reference numerals refer to like elements throughout the specification. The expression "and/or" includes any and all combinations of one or more of the associated listed items.
It should be noted that in this specification, the expressions first, second, third, etc. are used only to distinguish one feature from another, and do not represent any limitation on the features. Thus, the first lens discussed below may also be referred to as the second lens or the third lens without departing from the teachings of the present application.
In the drawings, the thickness, size, and shape of the lens have been slightly exaggerated for convenience of explanation. In particular, the shapes of the spherical or aspherical surfaces shown in the drawings are shown by way of example. That is, the shape of the spherical surface or the aspherical surface is not limited to the shape of the spherical surface or the aspherical surface shown in the drawings. The figures are purely diagrammatic and not drawn to scale.
Herein, the paraxial region refers to a region near the optical axis. If the lens surface is convex and the convex position is not defined, it means that the lens surface is convex at least in the paraxial region; if the lens surface is concave and the concave position is not defined, it means that the lens surface is concave at least in the paraxial region. The surface of each lens closest to the object is called the object side surface of the lens, and the surface of each lens closest to the imaging surface is called the image side surface of the lens.
It will be further understood that the terms "comprises," "comprising," "has," "having," "includes" and/or "including," when used in this specification, specify the presence of stated features, elements, and/or components, but do not preclude the presence or addition of one or more other features, elements, components, and/or groups thereof. Moreover, when a statement such as "at least one of" appears after a list of listed features, the entirety of the listed features is modified rather than modifying individual elements in the list. Furthermore, when describing embodiments of the present application, the use of "may" mean "one or more embodiments of the present application. Also, the term "exemplary" is intended to refer to an example or illustration.
Unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this application belongs. It will be further understood that terms, such as those defined in commonly used dictionaries, should be interpreted as having a meaning that is consistent with their meaning in the context of the relevant art and will not be interpreted in an idealized or overly formal sense unless expressly so defined herein.
It should be noted that the embodiments and features of the embodiments in the present application may be combined with each other without conflict. The present application will be described in detail below with reference to the embodiments with reference to the attached drawings.
The features, principles and other aspects of the present invention are described in detail below.
The optical imaging lens according to an exemplary embodiment of the present application may include, for example, five lenses having optical powers, i.e., a first lens, a second lens, a third lens, a fourth lens, and a fifth lens. The five lenses are arranged in sequence from the object side to the image side along the optical axis.
In an exemplary embodiment, the first lens has a positive optical power; the second lens has negative focal power; the third lens may have a positive optical power or a negative optical power; the fourth lens has positive focal power; the fifth lens has negative focal power, and the object side surface of the fifth lens is a concave surface. The positive focal power of the first lens and the negative focal power of the second lens are beneficial to reducing the FNO of the shooting lens group and simultaneously enabling the light rays to have better convergence effect; the fourth lens with positive focal power and the fifth lens with negative focal power, wherein the object side surface of the fifth lens is a concave surface, so that the focal power of the camera lens group can be reasonably distributed and prevented from being excessively concentrated on one or two lenses, marginal rays can be well converged on an imaging surface, the imaging area of the camera lens group can be increased, coma of the camera lens group can be corrected, and the camera lens group has good imaging quality.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression f/EPD <1.9, where f is an effective focal length of the optical imaging lens and EPD is an entrance pupil diameter of the optical imaging lens. By controlling the f/EPD to be less than 1.9, the light flux of the lens can be effectively increased, so that the lens has higher relative illumination, the resolving power of the lens in a dark environment can be well improved, and the lens has higher practicability. More specifically, f and EPD satisfy: f/EPD is more than or equal to 1.84 and less than or equal to 1.87.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression TTL/ImgH ≦ 1.25, where TTL is an on-axis distance from an object-side surface of the first lens element to an imaging surface, and ImgH is half a diagonal length of an effective pixel area on the imaging surface. By controlling TTL/ImgH to be less than or equal to 1.25, the problem of overlong integral size of the camera lens group caused by over-thickness of the first lens can be avoided while the basic imaging height is ensured, and the characteristic of keeping the camera lens group in an ultra-small size is facilitated. More specifically, the following conditions can be satisfied between TTL and ImgH: TTL/ImgH is more than or equal to 1.20 and less than or equal to 1.25.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 1.7< (f1+ f4)/f <2.2, where f1 is an effective focal length of the first lens, f4 is an effective focal length of the fourth lens, and f is an effective focal length of the optical imaging lens. By controlling the first lens, the fourth lens and the effective focal length of the system, on one hand, the size of the system can be effectively reduced, on the other hand, the focal power of the system is prevented from being excessively concentrated on the first lens and the fourth lens, and meanwhile, the spherical aberration contribution amounts of the two lenses can be controlled in a reasonable range, so that the system can obtain better imaging quality. More specifically, f1, f4 and f satisfy: (f1+ f4)/f is not more than 1.80 and not more than 2.18.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 2.4< f2/f5<4.2, where f2 is an effective focal length of the second lens and f5 is an effective focal length of the fifth lens. By controlling the effective focal length of the second lens and the optical power of the fifth lens, while avoiding excessive concentration of optical power in the fifth lens, it helps to reduce the sensitivity of the fifth lens so that it has better processing feasibility. More specifically, f2 and f5 satisfy: f2/f5 is more than or equal to 2.41 and less than or equal to 4.11.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 2.0< (R3+ R4)/(R3-R4) <2.6, where R3 is a radius of curvature of an object-side surface of the second lens and R4 is a radius of curvature of an image-side surface of the second lens. The curvature radius of the object side surface of the second lens and the curvature radius of the image side surface of the second lens are controlled, so that the optical focal length value of the second lens is reduced, the light is better converged for main use, the improvement of the image quality of the system is facilitated, and the improvement of the relative illumination of the system is greatly facilitated; meanwhile, the second lens can keep good processing manufacturability, and the practicability of the lens group is improved. More specifically, R3 and R4 satisfy: 2.06 is less than or equal to (R3+ R4)/(R3-R4) is less than or equal to 2.54.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 0.6< (R2-R1)/(R2+ R1) <0.9, where R2 is a radius of curvature of the image-side surface of the first lens and R1 is a radius of curvature of the object-side surface of the first lens. By reasonably distributing the curvature radiuses of the object side surface and the image side surface of the first lens, astigmatism and coma between the first lens and the rear lenses can be effectively balanced. More specifically, R1 and R2 satisfy: the ratio of (R2-R1)/(R2+ R1) is not more than 0.66 and not more than 0.72.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 0.5< CT1/(CT2+ CT3) <0.9, where CT1 is a central thickness of the first lens on the optical axis, CT2 is a central thickness of the second lens on the optical axis, and CT3 is a central thickness of the third lens on the optical axis. The center thicknesses of the first lens, the second lens and the third lens on the optical axis are reasonably distributed, so that the size of the system is reduced, and the spherical aberration of the system is reduced; and the distortion amount of the system can be effectively reduced by controlling the medium thicknesses of the first lens, the second lens and the third lens within a reasonable range, and the ghost risk caused by the internal reflection of light is reduced. More specifically, CT1, CT2 and CT3 satisfy: 0.54-0. 1/(CT2+ CT3) -0.85.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 1.5< T34/(T12+ T23) <2.1, where T34 is an air space between the third lens and the fourth lens on the optical axis, T12 is an air space between the first lens and the second lens on the optical axis, and T23 is an air space between the second lens and the third lens on the optical axis. Through the air interval of rational control first lens and second lens on the optical axis and the air interval of second lens and third lens on the optical axis, be favorable to the miniaturization of system, and reduce the ghost image risk that second lens object side brought, cooperate the air interval of third lens and fourth lens on the optical axis to reduce the colour difference of system effectively, can guarantee processing and equipment characteristic, be favorable to slowing down light deflection simultaneously, adjust the field curvature of the lens group of making a video recording, reduce the degree of sensitivity, thereby improve the yield. More specifically, T12, T23 and T34 satisfy: T34/(T12+ T23) is not less than 1.52 and not more than 2.05.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 3.1mm < f × tan (1/2FOV) <3.7mm, where f is an effective focal length of the optical imaging lens and FOV is a maximum angle of view of the optical imaging lens. The effective focal length of the optical imaging lens and the maximum field angle of the optical imaging lens are controlled, so that the field angle of an imaging group is controlled within a reasonable range, the imaging height of a system is improved, the overlarge aberration of a marginal field is avoided, the size of the aperture of the camera lens group is increased, and the characteristics of wide imaging range and high imaging quality are achieved. More specifically, f and FOV satisfy: f multiplied by tan (1/2FOV) is less than or equal to 3.53mm and is less than or equal to 3.29 mm.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 1.2< f12/f <1.7, where f12 is a composite focal length of the first and second lenses, and f is an effective focal length of the optical imaging lens. By reasonably controlling the conditional expression within a reasonable range, on one hand, the size of the system can be effectively reduced, the focal power of the system is prevented from being excessively concentrated on the first lens and the second lens, on the other hand, the spherical aberration contribution amounts of the two lenses can be controlled within a reasonable range, and better resolving power is obtained. More specifically, f12 and f satisfy: f12/f is more than or equal to 1.46 and less than or equal to 1.67.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 1.4< ET5/CT5<2.3, where ET5 is an edge thickness of the fifth lens and CT5 is a center thickness of the fifth lens on an optical axis. By controlling the central thickness of the fifth lens on the optical axis and the edge thickness of the fifth lens, the difficulty in processing caused by over-thinness of the fifth lens is avoided, the risk of ghost images of the system can be effectively reduced, and the processing manufacturability is improved. More specifically, ET5 and CT5 satisfy: ET5/CT5 is more than or equal to 1.44 and less than or equal to 2.20.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 1.2< CT4/ET4<1.8, where CT4 is a central thickness of the fourth lens on an optical axis and ET4 is an edge thickness of the fourth lens. By controlling the central thickness of the fourth lens on the optical axis and the edge thickness of the fourth lens, performance degradation caused by over-thickness of the fourth lens is avoided, and manufacturability of fourth lens processing forming is improved. More specifically, the following conditions are satisfied between CT4 and ET 4: CT4/ET4 is more than or equal to 1.28 and less than or equal to 1.75.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 0.2< SAG52/SAG51<0.7, where SAG52 is an on-axis distance between an intersection of the image-side surface of the fifth lens and the optical axis and an effective radius vertex of the image-side surface of the fifth lens, and SAG51 is an on-axis distance between an intersection of the object-side surface of the fifth lens and the optical axis and an effective radius vertex of the object-side surface of the fifth lens. Through the rise size of the object side face and the image side face of the rational distribution fifth lens, the fifth lens is prevented from being too bent, the processing difficulty is reduced, the spherical aberration of the camera lens group is reduced, and the spherical aberration of the middle view field and the coma of the edge view field are improved. More specifically, SAG52 and SAG51 satisfy: 0.24 is less than or equal to SAG52/SAG51 is less than or equal to 0.68.
In an exemplary embodiment, the optical imaging lens of the present application may satisfy the conditional expression 1.2< DT32/DT22<1.5, where DT32 is an effective half aperture of an image side surface of the third lens and DT22 is an effective half aperture of an image side surface of the second lens. By controlling the effective semi-caliber of the image side surface of the third lens and the effective semi-caliber of the image side surface of the second lens, the difference of the effective radiuses of the image side surfaces of the second lens and the third lens can be effectively prevented from being overlarge, the lens processing and forming are facilitated, and the stability of the performance of the camera lens group is improved. More specifically, DT32 and DT22 satisfy: DT32/DT22 of more than or equal to 1.24 and less than or equal to 1.36.
In an exemplary embodiment, the optical imaging lens may further include at least one diaphragm. The stop may be disposed at an appropriate position as needed, for example, between the object side and the first lens. Optionally, the optical imaging lens may further include a filter for correcting color deviation and/or a protective glass for protecting a photosensitive element on the imaging surface.
The optical imaging lens according to the above-described embodiment of the present application may employ a plurality of lenses, for example, five lenses as described above. The optical imaging lens has the advantages that the optical focal power and the surface type of each lens, the central thickness of each lens, the on-axis distance between each lens and the like are reasonably distributed, so that the optical imaging lens has a larger imaging image surface, has ultrahigh cost performance, can provide a larger aperture, has unusual imaging quality even in a dark environment, becomes a flat replacement for six or seven lenses, and simultaneously can provide enough space for subsequent related adjustment due to the unique lens model, so that the related structure and the assembling process are more flexible.
However, it will be appreciated by those skilled in the art that the number of lenses constituting an optical imaging lens may be varied to achieve the various results and advantages described in the present specification without departing from the claimed subject matter. For example, although five lenses are exemplified in the embodiment, the optical imaging lens is not limited to include five lenses. The optical imaging lens may also include other numbers of lenses, if desired.
Specific embodiments of an optical imaging lens suitable for the above-described embodiments are further described below with reference to the drawings.
Example one
Fig. 1 is a schematic structural diagram of an optical imaging lens according to a first embodiment of the present invention, as shown in fig. 1, the camera lens assembly includes, in order from an object side to an image side, a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, an optical filter E6, and an imaging plane S13.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2; the second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4; the third lens element E3 has positive power, and has a concave object-side surface S5 and a convex image-side surface S6; the fourth lens element E4 has positive power, and has a concave object-side surface S7 and a convex image-side surface S8; the fifth lens element E5 has negative power, and has a concave object-side surface S9 and a concave image-side surface S10. The light from the object sequentially passes through the respective surfaces S1 to S12 and is finally imaged on the imaging surface S13.
Table 1 shows the basic parameters of the optical imaging lens of the first embodiment, wherein the curvature radius, the thickness, and the focal length are in millimeter units.
Flour mark Surface type Radius of curvature Thickness of Focal length Refractive index Coefficient of dispersion Coefficient of cone
OBJ Spherical surface All-round All-round
STO Spherical surface All-round -0.2933
S1 Aspherical surface 1.6354 0.6041 3.65 1.55 56.1 -0.3622
S2 Aspherical surface 7.9248 0.0684 -21.5845
S3 Aspherical surface 7.3020 0.2800 -8.70 1.67 20.4 51.9333
S4 Aspherical surface 3.1808 0.3379 6.8233
S5 Aspherical surface -181.4709 0.4283 16.64 1.55 56.1 -99.0000
S6 Aspherical surface -8.6576 0.6157 -87.5001
S7 Aspherical surface -24.5527 0.6004 2.98 1.55 56.1 -94.1600
S8 Aspherical surface -1.5411 0.3339 -2.3073
S9 Aspherical surface -27.2074 0.4652 -2.12 1.54 55.7 -47.7766
S10 Aspherical surface 1.1936 0.2870 -6.0633
S11 Spherical surface All-round 0.2100 1.52 64.2
S12 Spherical surface All-round 0.3711
S13 Spherical surface All-round
TABLE 1
In embodiment 1, the value of the total effective focal length f of the optical imaging lens is 3.69mm, the value of the on-axis distance TTL from the object side surface S1 of the first lens E1 to the imaging surface S15 is 4.60mm, and the value of ImgH, which is half the diagonal length of the effective pixel area on the imaging surface S15, is 3.70 mm.
In the first embodiment, the effective focal length f of the optical imaging lens and the entrance pupil diameter EPD of the optical imaging lens have a relationship f/EPD of 1.87, which satisfies f/EPD < 1.9.
In the first embodiment, the on-axis distance TTL from the object-side surface of the first lens element to the imaging surface and half ImgH of the diagonal length of the effective pixel area on the imaging surface have a relationship of TTL/ImgH equal to 1.24, which satisfies TTL/ImgH ≦ 1.25.
In the first embodiment, the effective focal length f1 of the first lens, the effective focal length f4 of the fourth lens, and the effective focal length of the optical imaging lens satisfy the relationship (f1+ f4)/f 1.80, which satisfies 1.7< (f1+ f4)/f < 2.2.
In the first embodiment, the effective focal length f2 of the second lens and the effective focal length f5 of the fifth lens have the relationship f2/f5 equal to 4.11, and 2.4< f2/f5<4.2 is satisfied.
In the first embodiment, the relationship between the radius of curvature R3 of the object-side surface of the second lens and the radius of curvature R4 of the image-side surface of the second lens (R3+ R4)/(R3-R4) is 2.54, and 2.0< (R3+ R4)/(R3-R4) <2.6 is satisfied.
In the first embodiment, the relationship between the radius of curvature R2 of the image-side surface of the first lens and the radius of curvature R1 of the object-side surface of the first lens (R2-R1)/(R2+ R1) is 0.66, and satisfies 0.6< (R2-R1)/(R2+ R1) < 0.9.
In the first embodiment, the central thickness CT1 of the first lens on the optical axis, the central thickness CT2 of the second lens on the optical axis, and the central thickness CT3 of the third lens on the optical axis satisfy the relation CT1/(CT2+ CT3) < 0.85, and 0.5< CT1/(CT2+ CT3) < 0.9.
In the first embodiment, the air space T34 between the third lens and the fourth lens on the optical axis, the air space T12 between the first lens and the second lens on the optical axis, and the air space T23 between the second lens and the third lens on the optical axis satisfy the relation T34/(T12+ T23) < 1.52, and 1.5< T34/(T12+ T23) < 2.1.
In the first embodiment, the relationship f × tan (1/2FOV) between the effective focal length f of the optical imaging lens and the maximum field angle FOV of the optical imaging lens is 3.53, and 3.1mm < f × tan (1/2FOV) <3.7mm is satisfied.
In the first embodiment, the combined focal length f12 of the first lens and the second lens and the effective focal length f of the optical imaging lens satisfy the relationship f12/f 1.46, which is 1.2< f12/f < 1.7.
In the first embodiment, the relationship between the edge thickness ET5 of the fifth lens and the optical axis center thickness CT5 of the fifth lens, ET5/CT5 is 1.44, and 1.4< ET5/CT5<2.3 is satisfied.
In the first embodiment, the central thickness CT4 of the fourth lens on the optical axis and the edge thickness ET4 of the fourth lens satisfy the relation CT4/ET4 equal to 1.75, and 1.2< CT4/ET4< 1.8.
In the present first embodiment, an on-axis distance SAG52 between the intersection point of the fifth lens image-side surface and the optical axis to the effective radius vertex of the fifth lens image-side surface and an on-axis distance SAG51 between the intersection point of the fifth lens object-side surface and the optical axis to the effective radius vertex of the fifth lens object-side surface, and the relationship SAG52/SAG51 is 0.65, satisfy 0.2< SAG52/SAG51< 0.7.
In the first embodiment, the effective half aperture DT32 of the image side surface of the third lens element and the effective half aperture DT22 of the image side surface of the second lens element have a relationship DT32/DT22 equal to 1.36, and 1.2< DT32/DT22<1.5 is satisfied.
In the first embodiment, the object-side surface and the image-side surface of any one of the first lens E1 to the fifth lens E5 are aspheric surfaces, and the surface shape x of each aspheric lens can be defined by, but is not limited to, the following aspheric surface formula:
wherein x is the rise of the distance from the aspheric surface vertex to the aspheric surface vertex when the aspheric surface is at the position with the height of h along the optical axis direction; c is the paraxial curvature of the aspheric surface, c being 1/R (i.e., paraxial curvature c is the inverse of radius of curvature R in table 1 above); k is the conic coefficient (given in table 1); ai is the correction coefficient of the i-th order of the aspherical surface.
Table 2 below shows the high-order term coefficients a4, a6, A8, a10, a12, a14, a16, a18, and a20 of each aspherical surface S1 to S10 that can be used for each aspherical lens in the first embodiment of the present application.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 6.3439E-03 1.6971E-02 -1.0983E-01 3.7930E-01 -8.1404E-01 9.9927E-01 -6.7353E-01 2.0286E-01 -1.2732E-02
S2 -1.0874E-01 8.3615E-02 3.1266E-01 -1.7720E+00 4.8372E+00 -8.3284E+00 8.7995E+00 -5.1630E+00 1.2785E+00
S3 -1.4146E-01 1.5682E-01 2.9774E-01 -1.6349E+00 3.9375E+00 -6.1878E+00 6.2957E+00 -3.7072E+00 9.3450E-01
S4 -6.5434E-02 2.5854E-01 -1.2804E+00 6.7251E+00 -2.2344E+01 4.5482E+01 -5.5402E+01 3.7159E+01 -1.0547E+01
S5 -1.1791E-01 -6.5044E-02 4.8935E-01 -2.7106E+00 8.4503E+00 -1.6296E+01 1.9082E+01 -1.2523E+01 3.5769E+00
S6 -1.2202E-01 1.2101E-01 -7.1211E-01 2.0889E+00 -3.8235E+00 4.3332E+00 -2.9481E+00 1.0934E+00 -1.6643E-01
S7 1.6125E-02 -8.6377E-02 1.4228E-01 -1.7642E-01 1.4001E-01 -7.1787E-02 2.2668E-02 -3.9206E-03 2.8094E-04
S8 7.7497E-02 -1.4470E-01 1.7370E-01 -1.2393E-01 5.5582E-02 -1.5747E-02 2.7249E-03 -2.6204E-04 1.0687E-05
S9 -2.3973E-01 1.3621E-01 -4.2312E-02 9.3942E-03 -1.6281E-03 2.1650E-04 -2.0138E-05 1.1282E-06 -2.8105E-08
S10 -1.0545E-01 6.2407E-02 -2.4916E-02 6.5259E-03 -1.0904E-03 1.0848E-04 -5.6923E-06 1.1094E-07 6.9731E-10
TABLE 2
Fig. 2 is an axial chromatic aberration curve of the optical imaging lens according to the first embodiment, which shows the convergent focus deviation of light rays with different wavelengths after passing through the lens. Fig. 3 shows astigmatism curves of the optical imaging lens in the first embodiment, which represent meridional field curvature and sagittal field curvature. Fig. 4 is a distortion curve of the optical imaging lens in the first embodiment, which shows distortion magnitude values corresponding to different image heights. Fig. 5 is a chromatic aberration of magnification curve of the optical imaging lens according to the first embodiment, which shows the deviation of different image heights of the light beam on the imaging surface after passing through the lens. As can be seen from fig. 2 to 5, the optical imaging lens of the first embodiment can achieve good imaging quality.
Example two
Fig. 6 is a schematic structural diagram of an optical imaging lens according to a second embodiment of the present invention, as shown in fig. 6, the camera lens assembly includes, in order from an object side to an image side, a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a filter E6, and an imaging plane S13.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2; the second lens element E2 has negative and positive power, and has a convex object-side surface S3 and a concave image-side surface S4; the third lens element E3 has positive power, and has a concave object-side surface S5 and a convex image-side surface S6; the fourth lens element E4 has positive power, and has a convex object-side surface S7 and a convex image-side surface S8; the fifth lens element E5 has negative power, and has a concave object-side surface S9 and a concave image-side surface S10. The light from the object sequentially passes through the respective surfaces S1 to S12 and is finally imaged on the imaging surface S13.
Table 3 shows the basic parameters of the optical imaging lens of the second embodiment, wherein the curvature radius, the thickness, and the focal length are in millimeter units.
Flour mark Surface type Radius of curvature Thickness of Focal length Refractive index Coefficient of dispersion Coefficient of cone
OBJ Spherical surface All-round All-round
STO Spherical surface All-round -0.2888
S1 Aspherical surface 1.8072 0.7033 3.97 1.55 56.1 -0.0983
S2 Aspherical surface 9.3432 0.0628 12.4863
S3 Aspherical surface 9.8155 0.3235 -8.80 1.67 20.4 54.4582
S4 Aspherical surface 3.6202 0.2973 4.9078
S5 Aspherical surface -281.4161 0.5750 15.55 1.55 56.1 -99.0000
S6 Aspherical surface -8.2484 0.6465 -45.7298
S7 Aspherical surface 32.6372 0.6066 3.66 1.55 56.1 -99.0000
S8 Aspherical surface -2.1128 0.4289 -1.2869
S9 Aspherical surface -24.8251 0.4210 -2.91 1.54 55.7 38.0846
S10 Aspherical surface 1.6745 0.2686 -5.7155
S11 Spherical surface All-round 0.2310 1.52 64.2
S12 Spherical surface All-round 0.4354
S13 Spherical surface All-round
TABLE 3
In embodiment 2, the value of the total effective focal length f of the optical imaging lens is 3.90mm, the value of the on-axis distance TTL from the object side surface S1 of the first lens E1 to the imaging surface S15 is 5.00mm, and the value of ImgH, which is half the diagonal length of the effective pixel area on the imaging surface S15, is 4.00 mm.
Table 4 below shows the high-order term coefficients a4, a6, A8, a10, a12, a14, a16, a18, and a20 for each aspherical surface S1-S10 that can be used for each aspherical lens in the second embodiment of the present application. Wherein each aspherical surface type can be defined by the formula (1) given in the above-described embodiment 1.
TABLE 4
Fig. 7 is a diagram illustrating an axial chromatic aberration curve of an optical imaging lens according to a second embodiment of the present application, which shows the convergent focus deviation of light rays with different wavelengths after passing through the lens. Fig. 8 shows astigmatism curves of an optical imaging lens according to a second embodiment of the present application, which represent meridional field curvature and sagittal field curvature. Fig. 9 is a distortion curve of the optical imaging lens according to the second embodiment of the present application, which shows distortion magnitude values corresponding to different image heights. Fig. 10 is a chromatic aberration of magnification curve of an optical imaging lens according to a second embodiment of the present application, which shows the deviation of different image heights of light rays on an imaging surface after passing through the lens. As can be seen from fig. 7 to 10, the optical imaging lens according to the second embodiment of the present application can achieve good imaging quality.
EXAMPLE III
Fig. 11 is a schematic structural diagram of an optical imaging lens according to a third embodiment of the present invention, as shown in fig. 11, the camera lens assembly includes, in order from an object side to an image side, a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a filter E6, and an imaging plane S13.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2; the second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4; the third lens element E3 has positive power, and has a convex object-side surface S5 and a convex image-side surface S6; the fourth lens element E4 has positive power, and has a concave object-side surface S7 and a convex image-side surface S8; the fifth lens element E5 has negative power, and has a concave object-side surface S9 and a concave image-side surface S10. The light from the object sequentially passes through the respective surfaces S1 to S12 and is finally imaged on the imaging surface S13.
Table 5 shows basic parameters of the optical imaging lens according to the third embodiment of the present application, where the radius of curvature, the thickness, and the focal length are all in millimeter units.
TABLE 5
In embodiment 3, the value of the total effective focal length f of the optical imaging lens is 3.52mm, the value of the on-axis distance TTL from the object side surface S1 to the imaging surface S15 of the first lens E1 is 4.70mm, and the value of ImgH, which is half the diagonal length of the effective pixel area on the imaging surface S15, is 3.86 mm.
Table 6 below shows the high-order term coefficients a4, a6, A8, a10, a12, a14, a16, a18, and a20 of each aspherical surface S1 to S10 that can be used for each aspherical lens in the third embodiment of the present application. Wherein each aspherical surface type can be defined by the formula (1) given in the above-described embodiment 1.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 6.7504E-03 -8.2402E-03 7.5604E-02 -2.1837E-01 3.6641E-01 -3.4602E-01 1.5692E-01 -9.9013E-03 -1.1882E-02
S2 -1.0588E-01 1.2458E-01 1.8473E-01 -9.6927E-01 1.8142E+00 -1.9066E+00 1.1165E+00 -3.2591E-01 3.4229E-02
S3 -1.5807E-01 2.9434E-01 -4.0482E-01 8.3475E-01 -2.0372E+00 3.4238E+00 -3.4173E+00 1.8215E+00 -3.9719E-01
S4 -6.7733E-02 1.2577E-01 -2.4142E-01 1.3294E+00 -5.0692E+00 1.0975E+01 -1.3589E+01 9.0523E+00 -2.5174E+00
S5 -1.0181E-01 1.6586E-01 -1.1541E+00 4.2433E+00 -9.7434E+00 1.3885E+01 -1.2002E+01 5.7268E+00 -1.1386E+00
S6 -9.3133E-02 4.9825E-02 -2.0619E-01 4.6632E-01 -7.5690E-01 7.9654E-01 -5.1065E-01 1.7849E-01 -2.5285E-02
S7 -4.8511E-02 1.1379E-01 -2.4477E-01 2.5192E-01 -1.5153E-01 5.2359E-02 -9.0799E-03 4.6774E-04 3.2881E-05
S8 4.6592E-02 -5.0205E-02 4.4408E-02 -4.4967E-02 3.4028E-02 -1.4691E-02 3.5384E-03 -4.4934E-04 2.3587E-05
S9 -1.5007E-01 1.1941E-02 3.5893E-02 -1.8233E-02 4.1577E-03 -5.0371E-04 3.0481E-05 -5.9159E-07 -1.1278E-08
S10 -1.1311E-01 5.6648E-02 -2.0217E-02 5.1788E-03 -9.3125E-04 1.1331E-04 -8.8248E-06 3.9460E-07 -7.6722E-09
TABLE 6
Fig. 12 is a diagram illustrating an axial chromatic aberration curve of an optical imaging lens according to a third embodiment of the present application, which shows the convergent focus deviation of light rays with different wavelengths after passing through the lens. Fig. 13 shows astigmatism curves of the optical imaging lens in the third embodiment of the present application, which represent meridional field curvature and sagittal field curvature. Fig. 14 shows distortion curves of the optical imaging lens according to the third embodiment of the present application, which show distortion magnitude values corresponding to different image heights. Fig. 15 is a chromatic aberration of magnification curve of an optical imaging lens according to a third embodiment of the present application, which shows the deviation of different image heights of light rays on an imaging surface after passing through the lens. As can be seen from fig. 12 to 15, the optical imaging lens according to the third embodiment of the present application can achieve good imaging quality.
Example four
Fig. 16 is a schematic structural diagram of an optical imaging lens according to a fourth embodiment of the present invention, as shown in fig. 16, the camera lens assembly includes, in order from an object side to an image side, a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a filter E6, and an imaging plane S13.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2; the second lens element E2 has negative and positive power, and has a convex object-side surface S3 and a concave image-side surface S4; the third lens element E3 has positive power, and has a concave object-side surface S5 and a convex image-side surface S6; the fourth lens element E4 has positive power, and has a concave object-side surface S7 and a convex image-side surface S8; the fifth lens element E5 has negative power, and has a concave object-side surface S9 and a concave image-side surface S10. The light from the object sequentially passes through the respective surfaces S1 to S12 and is finally imaged on the imaging surface S13.
Table 7 shows basic parameters of the optical imaging lens according to the fourth embodiment of the present application, where the radius of curvature, the thickness, and the focal length are all in millimeter units.
Flour mark Surface type Radius of curvature Thickness of Focal length Refractive index Coefficient of dispersion Coefficient of cone
OBJ Spherical surface All-round All-round
STO Spherical surface All-round -0.3577
S1 Aspherical surface 1.7722 0.5534 3.79 1.55 56.1 0.0244
S2 Aspherical surface 10.9529 0.0527 25.9236
S3 Aspherical surface 9.1892 0.4966 -7.53 1.67 20.4 36.3211
S4 Aspherical surface 3.1738 0.3568 5.2208
S5 Aspherical surface -76.2671 0.5178 12.03 1.55 56.1 99.0000
S6 Aspherical surface -6.0631 0.7649 8.7880
S7 Aspherical surface -99.2193 0.5889 4.67 1.55 56.1 99.0000
S8 Aspherical surface -2.4920 0.5480 -1.3429
S9 Aspherical surface -38.7224 0.4283 -3.00 1.54 55.7 75.8506
S10 Aspherical surface 1.6835 0.3127 -4.3272
S11 Spherical surface All-round 0.2415 1.52 64.2
S12 Spherical surface All-round 0.1883
S13 Spherical surface All-round
TABLE 7
In embodiment 4, the value of the total effective focal length f of the optical imaging lens is 3.97mm, the value of the on-axis distance TTL from the object side surface S1 of the first lens E1 to the imaging surface S15 is 5.05mm, and the value of ImgH, which is half the diagonal length of the effective pixel area on the imaging surface S15, is 4.20 mm.
Table 8 below shows the high-order term coefficients a4, a6, A8, a10, a12, a14, a16, a18, and a20 of each aspherical surface S1 to S10 that can be used for each aspherical lens in the fourth embodiment of the present application. Wherein each aspherical surface type can be defined by the formula (1) given in the above-described embodiment 1.
TABLE 8
Fig. 17 is a diagram illustrating an axial chromatic aberration curve of an optical imaging lens according to a fourth embodiment of the present application, which shows the convergent focus deviation of light rays with different wavelengths after passing through the lens. Fig. 18 shows astigmatism curves of the optical imaging lens system according to the fourth embodiment of the present application, which represent meridional field curvature and sagittal field curvature. Fig. 19 is a distortion curve of the optical imaging lens according to the fourth embodiment of the present application, which shows distortion magnitude values corresponding to different image heights. Fig. 20 is a chromatic aberration of magnification curve of an optical imaging lens according to a fourth embodiment of the present application, which shows the deviation of different image heights of light rays on an imaging surface after passing through the lens. As can be seen from fig. 17 to 20, the optical imaging lens according to the fourth embodiment of the present application can achieve good imaging quality.
EXAMPLE five
Fig. 21 is a schematic structural diagram of an optical imaging lens according to a fifth embodiment of the present invention, and as shown in fig. 21, the camera lens assembly includes, in order from an object side surface to an image side surface, a stop STO, a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, a fifth lens E5, a filter E6, and an image plane S13.
The first lens element E1 has positive power, and has a convex object-side surface S1 and a concave image-side surface S2; the second lens element E2 has negative power, and has a convex object-side surface S3 and a concave image-side surface S4; the third lens element E3 has positive power, and has a concave object-side surface S5 and a convex image-side surface S6; the fourth lens element E4 has positive power, and has a concave object-side surface S7 and a convex image-side surface S8; the fifth lens element E5 has negative power, and has a concave object-side surface S9 and a concave image-side surface S10. The light from the object sequentially passes through the respective surfaces S1 to S12 and is finally imaged on the imaging surface S13.
Table 9 shows basic parameters of the optical imaging lens according to the fifth embodiment of the present application, where the radius of curvature, the thickness, and the focal length are all in millimeter units.
TABLE 9
In embodiment 5, the value of the total effective focal length f of the optical imaging lens is 3.81mm, the value of the on-axis distance TTL from the object side surface S1 of the first lens E1 to the imaging surface S15 is 4.90mm, and the value of ImgH, which is half the diagonal length of the effective pixel area on the imaging surface S15, is 4.10 mm.
The following table 10 shows the high-order term coefficients a4, a6, A8, a10, a12, a14, a16, a18, and a20 of each aspherical surface S1 to S10 that can be used for each aspherical lens in the fifth embodiment of the present application. Wherein each aspherical surface type can be defined by the formula (1) given in the above-described embodiment 1.
Flour mark A4 A6 A8 A10 A12 A14 A16 A18 A20
S1 1.8855E-03 1.3456E-02 -6.0755E-02 2.2793E-01 -4.9702E-01 6.6035E-01 -5.2483E-01 2.3123E-01 -4.3680E-02
S2 -8.8433E-02 1.3578E-01 -1.9512E-01 4.7113E-01 -9.9552E-01 1.2978E+00 -9.6698E-01 3.7430E-01 -5.8077E-02
S3 -1.0200E-01 1.3838E-01 -1.8259E-01 5.0690E-01 -1.2593E+00 1.8671E+00 -1.5741E+00 6.9552E-01 -1.2448E-01
S4 -3.8501E-02 6.3521E-02 -1.3021E-01 3.8424E-01 -8.0929E-01 1.0782E+00 -8.7162E-01 3.9608E-01 -7.7017E-02
S5 -8.4313E-02 1.5098E-02 -5.1307E-02 -2.9063E-01 1.5079E+00 -3.3166E+00 3.8640E+00 -2.3509E+00 5.9072E-01
S6 -4.9948E-02 -2.0084E-01 1.6075E+00 -8.3913E+00 2.8864E+01 -6.9131E+01 1.1839E+02 -1.4669E+02 1.3152E+02
S7 -2.9919E-02 5.1727E-02 -1.0875E-01 4.3981E-02 1.5179E-01 -3.3437E-01 3.5185E-01 -2.3213E-01 1.0205E-01
S8 3.7581E-02 -5.8106E-02 1.5788E-01 -3.2895E-01 4.2982E-01 -3.6553E-01 2.0878E-01 -8.1363E-02 2.1684E-02
S9 -1.1261E-01 -8.1362E-02 1.8709E-01 -1.6986E-01 9.8901E-02 -3.9882E-02 1.1463E-02 -2.3819E-03 3.5905E-04
S10 -2.8591E-02 -9.0651E-02 1.2495E-01 -8.4180E-02 3.5870E-02 -1.0487E-02 2.1841E-03 -3.2969E-04 3.6188E-05
Watch 10
Fig. 22 is a diagram illustrating an axial chromatic aberration curve of an optical imaging lens according to a fifth embodiment of the present application, which shows the convergent focus deviation of light rays with different wavelengths after passing through the lens. Fig. 23 shows astigmatism curves of an optical imaging lens according to a fifth embodiment of the present application, which represent meridional field curvature and sagittal field curvature. Fig. 24 shows distortion curves of the optical imaging lens in the fifth embodiment of the present application, which show distortion magnitude values corresponding to different image heights. Fig. 25 is a chromatic aberration of magnification curve of an optical imaging lens according to a fifth embodiment of the present application, which shows the deviation of different image heights of light rays on an imaging surface after passing through the lens. As can be seen from fig. 22 to 25, the optical imaging lens according to the fifth embodiment of the present application can achieve good imaging quality.
In summary, in examples 1 to 5 of the present application, the optical parameters are as follows:
example parameters 1 2 3 4 5
f1(mm) 3.65 3.97 3.67 3.79 3.74
f2(mm) -8.70 -8.80 -7.59 -7.53 -7.40
f3(mm) 16.64 15.55 10.49 12.03 11.43
f4(mm) 2.98 3.66 3.80 4.67 4.58
f5(mm) -2.12 -2.91 -2.83 -3.00 -3.08
f(mm) 3.69 3.90 3.52 3.97 3.81
TTL(mm) 4.60 5.00 4.70 5.05 4.90
ImgH(mm) 3.70 4.00 3.86 4.20 4.10
TABLE 11
In examples 1 to 5 of the present application, the respective conditional expressions satisfy the conditions of the following table 12:
conditions/examples 1 2 3 4 5
f/EPD 1.87 1.87 1.85 1.87 1.84
TTL/ImgH 1.24 1.25 1.22 1.20 1.20
(f1+f4)/f 1.80 1.96 2.12 2.13 2.18
f2/f5 4.11 3.03 2.68 2.51 2.41
(R3+R4)/(R3-R4) 2.54 2.17 2.19 2.06 2.07
(R2-R1)/(R2+R1) 0.66 0.68 0.68 0.72 0.71
CT1/(CT2+CT3) 0.85 0.78 0.68 0.55 0.54
T34/(T12+T23) 1.52 1.80 1.93 1.87 2.05
f×tan(1/2FOV)(mm) 3.53 3.48 3.29 3.51 3.42
f12/f 1.46 1.56 1.67 1.54 1.59
ET5/CT5 1.44 2.20 1.64 1.66 2.12
CT4/ET4 1.75 1.29 1.39 1.28 1.37
SAG52/SAG51 0.65 0.24 0.62 0.68 0.42
DT32/DT22 1.36 1.28 1.36 1.33 1.24
TABLE 12
The present application also provides an imaging device, which is provided with an electron photosensitive element to form an image, wherein the electron photosensitive element may be a Charge Coupled Device (CCD) or a Complementary Metal Oxide Semiconductor (CMOS). The imaging device may be a stand-alone imaging device such as a digital camera, or may be an imaging module integrated on a mobile electronic device such as a mobile phone. The imaging device is equipped with the optical imaging lens described above.
The above description is only a preferred embodiment of the application and is illustrative of the principles of the technology employed. It will be understood by those skilled in the art that the scope of the present invention is not limited to the specific combination of the above-mentioned features, but also covers other embodiments formed by any combination of the above-mentioned features or their equivalents without departing from the spirit of the present invention. For example, the above features may be replaced with (but not limited to) features having similar functions disclosed in the present application.

Claims (14)

1. An optical imaging lens, in order from an object side to an image side along an optical axis, comprising:
a first lens having a positive optical power;
a second lens having a negative optical power;
a third lens having optical power;
a fourth lens having a positive optical power;
a fifth lens element having a negative refractive power, the object-side surface of which is concave;
the effective focal length f of the optical imaging lens, the entrance pupil diameter EPD of the optical imaging lens, the on-axis distance TTL from the object side surface of the first lens to the imaging surface and the half of the diagonal length ImgH of the effective pixel area on the imaging surface satisfy the following conditions: f/EPD < 1.9; and TTL/ImgH is less than or equal to 1.25.
2. The optical imaging lens of claim 1, wherein the effective focal length f1 of the first lens, the effective focal length f4 of the fourth lens, and the effective focal length f of the optical imaging lens satisfy: 1.7< (f1+ f4)/f < 2.2.
3. The optical imaging lens of claim 1, wherein an effective focal length f2 of the second lens and an effective focal length f5 of the fifth lens satisfy: 2.4< f2/f5< 4.2.
4. The optical imaging lens of claim 1, wherein a radius of curvature R3 of the object-side surface of the second lens and a radius of curvature R4 of the image-side surface of the second lens satisfy: 2.0< (R3+ R4)/(R3-R4) < 2.6.
5. The optical imaging lens of claim 1, wherein a radius of curvature R2 of the first lens image side surface and a radius of curvature R1 of the first lens object side surface satisfy: 0.6< (R2-R1)/(R2+ R1) < 0.9.
6. The optical imaging lens according to claim 1, wherein a center thickness CT1 of the first lens on an optical axis, a center thickness CT2 of the second lens on the optical axis, and a center thickness CT3 of the third lens on the optical axis satisfy: 0.5< CT1/(CT2+ CT3) < 0.9.
7. The optical imaging lens of claim 1, wherein an air interval T34 on an optical axis between the third lens and the fourth lens, an air interval T12 on an optical axis between the first lens and the second lens, and an air interval T23 on an optical axis between the second lens and the third lens satisfy: 1.5< T34/(T12+ T23) < 2.1.
8. The optical imaging lens of claim 1, wherein the effective focal length f of the optical imaging lens and the maximum field angle FOV of the optical imaging lens satisfy: 3.1mm < f × tan (1/2FOV) <3.7 mm.
9. The optical imaging lens of claim 1, wherein a combined focal length f12 of the first lens and the second lens and an effective focal length f of the optical imaging lens satisfy: 1.2< f12/f < 1.7.
10. The optical imaging lens of claim 1, wherein an edge thickness ET5 of the fifth lens and a center thickness CT5 of the fifth lens on an optical axis satisfy: 1.4< ET5/CT5< 2.3.
11. The optical imaging lens of claim 1, wherein the fourth lens has a center thickness CT4 on an optical axis and an edge thickness ET4 of the fourth lens that satisfy: 1.2< CT4/ET4< 1.8.
12. The optical imaging lens of claim 1, wherein an on-axis distance SAG52 from the intersection point of the fifth lens image side surface and the optical axis to the effective radius vertex of the fifth lens image side surface and an on-axis distance SAG51 from the intersection point of the fifth lens object side surface and the optical axis to the effective radius vertex of the fifth lens object side surface satisfy: 0.2< SAG52/SAG51< 0.7.
13. The optical imaging lens of claim 1, wherein the effective half aperture DT32 of the image side surface of the third lens and the effective half aperture DT22 of the image side surface of the second lens satisfy: 1.2< DT32/DT22< 1.5.
14. An optical imaging lens, in order from an object side to an image side along an optical axis, comprising:
a first lens having a positive optical power;
a second lens having a negative optical power;
a third lens having optical power;
a fourth lens having a positive optical power;
a fifth lens element having a negative refractive power, the object-side surface of which is concave;
wherein an effective focal length f2 of the second lens and an effective focal length f5 of the fifth lens satisfy: 2.4< f2/f5< 4.2; and an air interval T34 of the third lens and the fourth lens on an optical axis, an air interval T12 of the first lens and the second lens on the optical axis, and an air interval T23 of the second lens and the third lens on the optical axis satisfy: 1.5< T34/(T12+ T23) < 2.1.
CN202021666841.3U 2020-08-12 2020-08-12 Optical imaging lens Active CN212515188U (en)

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