Wide-angle lens

Information

  • Patent Grant
  • 11841549
  • Patent Number
    11,841,549
  • Date Filed
    Wednesday, August 5, 2020
    4 years ago
  • Date Issued
    Tuesday, December 12, 2023
    a year ago
Abstract
The present disclosure provides a wide-angle lens, including a first lens group having a negative focal power, a second lens group having a positive focal power, and an aperture stop disposed between the first lens group and the second lens group. The first lens group, from the object side to the imaging surface, sequentially includes a meniscus-shaped first lens having a negative focal power, a second lens having a negative focal power, and a third lens having a positive focal power. A concave surface of the first lens faces the imaging surface, and a concave surface of the second lens faces the imaging surface.
Description
TECHNICAL FIELD

The present disclosure relates to a technical filed of cameras, in particular to a wide-angle lens.


BACKGROUND

With development of automatic driving functions, a wide-angle lens such as a vehicle-mounted lens, which serves as a key component of automatic driving assistant system, has developed rapidly, and requirements for the wide-angle lens also become higher.


Compared with an ordinary optical lens, the vehicle-mounted lens in the automatic driving assistant system has special requirements. For example, the vehicle-mounted lens requires a front port diameter to be as small as possible, a strong light transmission capability, and requires the vehicle-mounted lens to be able to adapt to light and darkness changes of an external environment, and accordingly has a high imaging clarity, such that the vehicle-mounted lens is able to effectively distinguish details of the external environment (such as highway signs, distant pedestrians and vehicles, etc.). Additionally, thermal stability of the vehicle-mounted lens should be nice, so that the vehicle-mounted lens has a good resolution at both high and low temperatures. Then the special requirements of automatic driving are satisfied.


However, most existing vehicle-mounted lenses are sensitive to changes of temperature, which is difficult to be used in a high-temperature environment or a low-temperature environment. In addition, the resolution of the existing vehicle-mounted lens in the high-temperature environment or the low-temperature environment is low, and is difficult to eliminate chromatic aberrations, resulting in blurred imaging, which is not conducive to practical applications.


SUMMARY

Based on this, an object of the present disclosure is to provide a wide-angle lens with high resolution in high and low temperature environments.


The present disclosure provides a wide-angle lens. From an object side to an imaging surface, the wide-angle lens sequentially includes: a first lens group having a negative focal power, a second lens group having a positive focal power, and an aperture stop disposed between the first lens group and the second lens group. The first lens group, from the object side to the imaging surface, sequentially includes a meniscus-shaped first lens having a negative focal power, a second lens having a negative focal power, and a third lens having a positive focal power. A concave surface of the first lens faces the imaging surface, and a concave surface of the second lens faces the imaging surface. The second lens group, from the object side to the imaging surface, sequentially includes a fourth lens having a positive focal power, a fifth lens having a positive focal power, a sixth lens having a negative focal power, and a seventh lens having a positive focal power. The fourth lens, the fifth lens, and the seventh lens are biconvex lenses, and the sixth lens is a biconcave lens. The fifth lens and the sixth lens are cemented a cemented lens. The first lens, the third lens, the fourth lens, the fifth lens, and the sixth lens are all glass spherical lenses. The second lens and the seventh lens are glass aspherical lenses, and optical center bits of the lenses in the first lens group and the second lens group are located on a same straight line.


Compared with the prior art, the present disclosure provides the wide-angle lens, making the fifth lens and the sixth lens to cement the cemented lens. The combined wide-angle lens is clearly imaged in a temperature ranges from −40° C. to +85° C. through adopting a combined structure of five glass spherical lenses and two glass aspherical lenses and reasonable focal power matching, therefore, wide-angle characteristic is satisfied, and the high resolution is kept in both high and low temperature environments.


Furthermore, the wide-angle lens satisfies the following expression: −0.85<φ2/y7<−0.6, wherein φ2 represents a refractive power of the second lens, and ω7 represents a refractive power of the seventh lens. The expression indicates that spherical aberration formed by the second lens and the seventh lens cancel each other, which is able to effectively improve an analysis force of the wide-angle lens.


Furthermore, the wide-angle lens satisfies the following expression: −5.5(dN/dT)5+(dN/dT)6<−4.5, wherein (dN/dT)5 represents a temperature coefficient of refractive index of the fifth lens, and (dN/dT)6 represents a temperature coefficient of refractive index of the sixth lens. The expression indicates that the fifth lens and the sixth lens effectively compensate influences of temperature changes on a focal length of the wide-angle lens, which further improves stability of the analysis force of the wide-angle lens at different temperatures.


Furthermore, the wide-angle lens satisfies the following expression: −15.5<(dN/dT)2+(dN/dT)7<−8.0, wherein (dN/dT)2 represents a temperature coefficient of refractive index of the second lens, and (dN/dT), represents a temperature coefficient of refractive index of the seventh lens. When this expression is satisfied, sensitivity of the wide-angle lens to the temperature is effectively reduced, and the stability of the analysis force of the wide-angle lens at different temperatures is further improved.


Furthermore, the wide-angle lens satisfies the following expression: −0.45<φ56<−0.2, wherein φ5 represents a refractive power of the fifth lens, and φ6 represents a refractive power of the sixth lens. When this expression is satisfied, color difference of the wide-angle lens can be effectively corrected, and the analysis force of the wide-angle lens is further improved.


Furthermore, the wide-angle lens satisfies the following expression: −0.63<φII/φ<−0.42, wherein φII represents a combined refractive power of the second lens group, and φ represents a refractive power of the wide-angle lens. When this expression is satisfied, astigmatism of the wide-angle lens can be effectively corrected, and the analysis force of the wide-angle lens is further improved.


Furthermore, the wide-angle lens satisfies the following expression: 0.95<|IH/(f*θ)|<1, wherein θ represents a maximum half-field angle of the wide-angle lens (representing as radians), IH represents an image height of the wide-angle lens when the half field angle is θ, and f represents an effective focal length of the wide-angle lens. This expression indicates radio of an actual image height of the wide-angle lens to an ideal image height of the wide-angle lens.


Furthermore, the wide-angle lens satisfies the following expressions: D1>D2>D3, where D1 represents the maximum diameter of the first lens, D2 represents the maximum diameter of the second lens, D3 represents the maximum diameter of the third lens.


Furthermore, the wide-angle lens satisfies the following expression: 1<T5/T7<2, wherein T5 represents the thickness of the fifth lens, T7 represents the thickness of the seventh lens.


Furthermore, the wide-angle: lens satisfies the following expressions: d12>d34>d67, wherein d12 represents the distance between the first lens and the second lens on the optical axis, d34 represents the distance between the third lens and the fourth lens on the optical axis, d67 represents the distance between the sixth lens and the seventh lens on the optical axis.


Furthermore, the wide-angle lens satisfies the following expression: −8<R9/R10<−2, wherein R9 represents a radius of curvature of an object side surface of the fourth lens, R10 represents a radius of curvature of an image side surface of the fourth lens.


Furthermore, the wide-angle lens satisfies the following expression: 0,3<R3/R5<1, wherein R3 represents a radius of curvature of an image side surface of the first lens, R5 represents a radius of curvature of an image side surface of the second lens.


Furthermore, the wide-angle lens satisfies the following expression: 3<R2/R3<5, wherein R2 represents a radius of curvature of an object side surface of the first lens, R3 represents a radius of curvature of an image side surface of the first lens.


Furthermore, surface shapes of the second lens and the seventh lens satisfy the following formula:







z
=



ch
2


1
+


1
-


(

1
+
K

)



c
2



h
2






+

Bh
4

+

Ch
6

+

Dh
8

+

Eh
10

+

Fh
12



,




wherein z represents a distance of a curved surface of the second lens or the seventh lens leaving away from a vertex of the curved surface in optical axis direction, c represents a curvature of the vertex of the curved surface, K represents a quadratic surface coefficient, h represents a distance from the optical axis to the curved surface, B, C, D, E, and F respectively represent a fourth order curve coefficient, a sixth order curve coefficient, an eighth order curve coefficient, a tenth order curve coefficient, and a twelfth order curve coefficient.


Compared with the prior art, the wide-angle lens at least has following advantages:


(1) The wide-angle lens adopts seven glass lenses, which is clearly imaged in the temperature range from −40° C. to +85° C. and is particularly suitable for camera fields such as motion cameras, vehicle-mounted cameras, which are used in a harsh environment.


(2)The wide-angle lens is clearly imaged through reasonable configuration of focal power combinations between the lenses, which can match with imaging chips with more than eight million pixels.


(3) A field angle of the wide-angle lens can reach 146 degrees, distortion of f-θ is effectively corrected, and the distortion of f-θ is controlled to be less than 5% thus, requirements of a large field angle are satisfied.


(4) An aperture number of the wide-angle lens is 1.8, which satisfies an imaging requirement of a darker environment.





BRIEF DESCRIPTION OF DRAWINGS


FIG. 1 is a schematic cross-sectional structural diagram of a wide-angle lens according to a first embodiment of the present disclosure.



FIG. 2 is a curve diagram of a field curve of the wide-angle lens according to the first embodiment of the present disclosure.



FIG. 3 is a curve diagram of axial aberration of the wide-angle lens according to the first embodiment of the present disclosure.



FIG. 4 is a curve diagram of vertical axis color difference of the wide-angle lens according to the first embodiment of the present disclosure.



FIG. 5 is a schematic cross-sectional structural diagram of a wide-angle lens according to a second embodiment of the present disclosure.



FIG. 6 is a curve diagram of a field curve of the wide-angle lens according to the second embodiment of the present disclosure.



FIG. 7 is a curve diagram of axial aberration of the wide-angle lens according to the second embodiment of the present disclosure.



FIG. 8 is a curve diagram of vertical axis color difference of the wide-angle lens according to the second embodiment of the present disclosure.



FIG. 9 is a schematic cross-sectional structural diagram of a wide-angle lens according to a third embodiment of the present disclosure.



FIG. 10 is a curve diagram of a field curve of the wide-angle lens according to the third embodiment of the present disclosure.



FIG. 11 is a curve diagram of axial aberration of the wide-angle lens according to the third embodiment of the present disclosure.



FIG. 12 is a curve diagram of vertical axis color difference of the wide-angle lens according to the third embodiment of the present disclosure.



FIG. 13 is a schematic cross-sectional structural diagram of a wide-angle lens according to a fourth embodiment of the present disclosure.



FIG. 14 is a curve diagram of a field curve of the wide-angle lens according to the fourth embodiment of the present disclosure.



FIG. 15 is a curve diagram of axial aberration of the wide-angle lens according to the fourth embodiment of the present disclosure.



FIG. 16 a curve diagram of vertical axis color difference of the wide-angle lens according to the fourth embodiment of the present disclosure.


Reference numerals of main components:




















Wide-angle lens
100
Aperture stop
ST



First lens
L1
Second lens
L2



Third lens
L3
Fifth lens
L5



Fourth lens
L4
Seventh lens
L7



Sixth lens
L6
Optical filter
G1










The present disclosure is further illustrated by the following detailed description in combination with the accompanying drawings.





DETAILED DESCRIPTION

The specific embodiments of the present disclosure are described in detail below with reference to the accompanying drawings. Several embodiments of the present disclosure are presented in the drawings. However, the disclosure may be embodied in many different forms and is not limited to the embodiments described herein. Rather, these embodiments are provided so that this disclosure is thorough comprehensive.


Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which the present disclosure belongs. The terminology used herein in the description of the present disclosure is for the purpose of describing particular embodiments only and is not intended to limit the present disclosure. As used herein, the term “and/or” includes any and all combinations of one or more of the associated listed items.


Embodiment 1

Referring to FIG. 1, FIG. 1 is a structural diagram of a wide-angle lens 100 according to a first embodiment of the present disclosure. The wide-angle lens 100, from an object side to an imaging surface, includes a first lens group having a negative focal power, a second lens group having a positive focal power, and an aperture stop ST disposed between the first lens group and the second lens group.


Specifically, the first lens group, from the object side to the imaging surface, sequentially includes a meniscus-shaped first lens L1 having a negative focal power, a second lens L2 having a negative focal power , and a third lens L3 having a positive focal power. A concave surface of the first lens faces the imaging surface, and a concave surface of the second lens faces the imaging surface. The second lens group, from the object side to the imaging surface, sequentially includes a fourth lens L4 having a positive focal power, a fifth lens L5 having a positive focal power, a sixth lens L6 having a negative focal power, and a seventh lens L7 having a positive focal power. The fourth lens L4, the fifth lens L5, and the seventh lens L7 are biconvex lenses; and the sixth lens L6 is a biconcave lens. The fifth lens L5 and the sixth lens L6 are cemented a cemented lens. The first lens L1, the third lens L3, the fourth lens L4, the fifth lens L5, and the sixth lens L6 are glass spherical lenses. The second lens L2 and the seventh lens L7 are glass aspherical lenses, and optical center bits of the lenses in the first lens group and the second lens group are all located on a same straight line.


The present disclosure provides the wide-angle lens, making the fifth lens L5 and the sixth lens L6 to cement the cemented lens. The first lens L1, the third lens L3, the fourth lens L4, the fifth lens L5, and the sixth lens L6 are prepared by using the glass spherical lenses. At the same time, the second lens L2 and the seventh lens L7 are prepared by using the glass aspherical lenses. The combined wide-angle lens 100 is clearly imaged in a temperature ranges from −40° C. to +85° C. through combination of each lens and reasonably setting focal power of each lens, therefore, wide-angle characteristic is satisfied, and the high resolution is kept in both high and low temperature environments.


Specifically, in one embodiment, surface shapes of the second lens and the seventh lens satisfy the following formula:







z
=



ch
2


1
+


1
-


(

1
+
K

)



c
2



h
2






+

Bh
4

+

Ch
6

+

Dh
8

+

Eh
10

+

Fh
12



,




wherein z represents a distance of a curved surface of the second lens or the seventh lens leaving away from a vertex of the curved surface in optical axis direction, c represents a curvature of the vertex of the curved surface, K represents a quadratic surface coefficient, h represents a distance from the optical axis to the curved surface, B, C, D, E, and F respectively represent a fourth order curve coefficient, a sixth order curve coefficient, an eighth order curve coefficient, a tenth order curve coefficient, and a twelfth order curve coefficient.


In the following different embodiments, relevant parameters of each lens of the wide-angle lens 100 are referred to parameter tables of the various embodiments.


Referring to FIG. 1, which is the wide-angle lens 100 provided in the first embodiment of the present disclosure, the relevant parameters of each lens in the wide-angle lens 100 are shown in Tables 1 -1 to 1-2.















TABLE 1-1






Surface
Surface
Curvature

Refractive
Abbe



number
type
radius-r
Thickness-d
index-Nd
number-Vd





















Subject to be
1
Spherical

Infinity




shot

surface






First lens
2
Spherical
14.451
0.979
1.911
35.3




surface







3
Spherical
3.798
3.597






surface






Second lens
4
Aspherical
−8.324
0.798
1.433
94.8




surface







5
Aspherical
7.810
0.848






surface






Third lens
6
Spherical
20.625
2.117
1.904
31.4




surface







7
Spherical
−13.682
2.575






surface






Aperture stop
8
Spherical

0.093






surface






Fourth lens
9
Spherical
61.748
2.492
1.697
55.5




surface







10
Spherical
−7.840
0.099






surface






Fifth lens
11
Spherical
10.398
3.478
1.593
68.5




surface






Sixth lens
13
Spherical
−5.061
0.800
1.762
26.6




surface







14
Spherical
8.170
0.747






surface






Seventh lens
15
Aspherical
8.184
3.452
1.566
71.3




surface







16
Aspherical
−7.616
0.30






surface






Optical filter
17
Spherical

0.400
1.517
64.21




surface







18
Spherical

3.125






surface






Flat Glass
19
Spherical

0.50
1.517
64.21




surface







20
Spherical

0.57






surface






Imaging surface
21
Spherical








surface


























TABLE 1-2





Surface








number
K
B
C
D
E
F





















4
0
  2.207e−3
−3.016e−4
  2.472e−5
−1.176e−6
  2.093e−8


5
−1.785
  3.264e−3
−3.616e−4
  3.318e−5
  1.892e−6
  4.638e−8


15
0.508
−1.033e−3
  4.246e−5
−3.607e−6
  2.243e−7
−3.651e−9


16
0.500
  6.032e−4
−2.078e−5
  4.484e−6
−3.126e−7
  1.008e−8









In one embodiment, a field curve, axial aberration and vertical axis color difference of the wide-angle lens 100 are respectively shown in FIGS. 2, 3, and 4. It can be seen that the field curve is in the range of (−0.05, +0.05), the axial aberration is in the range of (−0.02,+0.02), and the vertical axis color difference is in the range of (−2.0,+10.0), which indicates that the field curve, aberration, and color difference is well corrected in one embodiment.


Embodiment 2

Referring to FIG. 5, which is a structural diagram of the wide-angle lens 100 provided in a second embodiment of the present disclosure and is substantially the same as a structure of the lens of embodiment 1, except that: (1) An object side surface of the second lens L2 is a convex surface, an image side surface of the second lens L2 is a concave surface. An object side surface of the third lens L3 is a convex surface, an image side surface of the third lens L3 is a concave surface; (2) the related parameters of each lens in the wide-angle lens of the embodiment are different, as shown in Table 2-1, and the parameters of each lens of spherical surfaces of one embodiment are shown in Table 2-2.















TABLE 2-1






Surface
Surface
Curvature
Thickness-
Refractive
Abbe



number
type
radius-r
d
index-Nd
number-Vd





















Subject to be shot
1
Spherical

Infinity






surface






First lens
2
Spherical
16.912
1.000
1.788
47.5




surface







3
Spherical
3.768
2.580






surface






Second lens
4
Aspherical
22.619
0.800
1.495
80.7




surface







5
Aspherical
4.875
0.879






surface






Third lens
6
Spherical
8.172
3.277
2.003
28.3




surface







7
Spherical
7.443
1.396






surface






Aperture stop
8
Spherical

0.100






surface






Fourth lens
9
Spherical
23.750
2.988
1.734
51.5




surface







10
Spherical
−5.814
0.103






surface






Fifth lens
11
Spherical
8.257
4.925
1.593
68.5




surface






Sixth lens
13
Spherical
−5.349
0.800
1.762
26.6




surface







14
Spherical
10.200
0.394






surface






Seventh lens
15
Aspherical
9.055
2.759
1.628
63.3




surface







16
Aspherical
−9.612
0.30






surface






Optical filter
17
Spherical

0.400
1.517
64.21




surface







18
Spherical

2.639






surface






Flat Glass
19
Spherical

0.50
1.517
64.21




surface







20
Spherical

0.57






surface






Imaging surface
21
Spherical








surface

























TABLE 2-2







Surface


















number
K
B
C
D
E
F
















4
29.621
  2.092e−3
−2.541e−4
  5.151e−6
  2.253e−7
−1.961e−8 


5
−0.542
  4.912e−3
−2.468e−4
  6.888e−6
−1.186e−7
  1.932e−8 


15
1.242
−6.274e−4
  6.758e−6
−8.588e−7
  5.150e−8
−1.864e−9 


16
−0.466
  8.965e−4
−7.414e−6
  1.311e−6
−2.518e−8
−2.906e−10









In the embodiment, the field curve, the axial aberration and the vertical axis color difference of the wide-angle lens 100 are respectively shown in FIGS. 6, 7, and 8. It can be seen that the field curve is in the range of (−0.05, +0.05), the axial aberration is in the range of (−0.02,+0.02), and the vertical axis color difference is in the range of (−3.5,+10.0), which indicates that the field curve, the aberration, and the color difference is well corrected in the embodiment.


Embodiment 3

Referring to FIG. 9, which is a structural diagram of the wide-angle lens 100 provided in a third embodiment of the present disclosure and is substantially the same as a structure of the lens of embodiment 2, except that the related parameters of each lens in the wide-angle lens of the embodiment are different, as shown in Table 3-1, and the parameters of each lens of spherical surfaces of one embodiment are shown in Table 3 -2.















TABLE 3-1






Surface
Surface
Curvature
Thickness-
Refractive
Abbe



number
type
radius-r
d
index-Nd
number-Vd





















Subject to be shot
1
Spherical

Infinity






surface






First lens
2
Spherical
16.107
0.976
1.804
46.7




surface







3
Spherical
3.846
2.934






surface






Second lens
4
Aspherical
−152.377
0.796
1.497
81.6




surface







5
Aspherical
5.882
0.674






surface






Third lens
6
Spherical
8.202
3.061
1.805
25.5




surface







7
Spherical
8.890
1.317






surface






Aperture stop
8
Spherical

0.032






surface






Fourth lens
9
Spherical
18.463
4.362
1.741
52.7




surface







10
Spherical
−6.779
0.040






surface






Fifth lens
11
Spherical
6.664
4.366
1.497
81.6




surface






Sixth lens
13
Spherical
−6.810
0.775
1.755
27.5




surface







14
Spherical
8.499
0.278






surface






Seventh lens
15
Aspherical
7.658
2.875
1.619
63.9




surface







16
Aspherical
−11.238
0.3






surface






Optical filter
17
Spherical

0.400
1.517
64.21




surface







18
Spherical

2.989






surface






Flat Glass
19
Spherical

0.50
1.517
64.21




surface







20
Spherical

0.57






surface






Imaging surface
21
Spherical








surface






















TABLE 3-2





Surface








number
K
B
C
D
E
F





















4
0
  2.222e−3
−3.250e−4
  2.465e−5
−1.110e−6
  1.905e−8 


5
0.617
  3.190e−3
−3.970e−4
  3.033e−5
−9.737e−7
−7.679e−9 


15
0.403
−9.900e−4
  4.412e−6
−5.675e−7
  3.958e−8
  3.211e−10


16
1.822
  6.820e−4
−3.345e−6
  1.520e−6
−8.079e−8
  3.840e−9 









In the embodiment, the field curve, the axial aberration and the vertical axis color difference of the wide-angle lens 100 are respectively shown in FIGS. 10, 11, and 12. It can be seen that the field curve is in the range of (−0.05, +0.05), the axial aberration is in the range of (−0.02,+0.02), and the vertical axis color difference is in the range of (−3.5,+10.0), which indicates that the field curve, the aberration, and the color difference is well corrected in the embodiment.


Embodiment 4

Referring to FIG. 13, which is a structural diagram of the wide-angle lens 100 provided in a fourth embodiment of the present disclosure and is substantially the same as a structure of the lens of embodiment 3, except that the related parameters of each lens in the wide-angle lens of the embodiment are different, as shown in Table 4-1, and the parameters of each lens of spherical surfaces of one embodiment are shown in Table 4 -2.















TABLE 4-1






Surface
Surface
Curvature
Thickness-
Refractive
Abbe



number
type
radius-r
d
index-Nd
number-Vd





















Subject to be shot
1
Spherical

Infinity






surface






First lens
2
Spherical
17.480
0.985
1.804
46.7




surface







3
Spherical
3.871
2.823






surface






Second lens
4
Aspherical
1914.498
0.857
1.433
94.8




surface







5
Aspherical
5.484
0.844






surface






Third lens
6
Spherical
8.248
3.466
1.805
75.5




surface







7
Spherical
7.851
1.066






surface






Aperture stop
8
Spherical

0.089






surface






Fourth lens
9
Spherical
18.665
3.745
1.741
52.7




surface







10
Spherical
−6.237
0.252






surface






Fifth lens
11
Spherical
6.799
4.319
1.497
81.6




surface






Sixth lens
13
Spherical
−6.592
0.794
1.755
27.5




surface







14
Spherical
8.827
0.307






surface






Seventh lens
15
Aspherical
8.463
2.839
1.628
63.3




surface







16
Aspherical
−10.148
0.3






surface






Optical filter
17
Spherical

0.400
1.517
64.21




surface







18
Spherical

2.862






surface






Flat Glass
19
Spherical

0.50
1.517
64.21




surface







20
Spherical

0.57






surface






Imaging surface
21
Spherical








surface






















TABLE 4-2





Surface








Number
K
B
C
D
E
F





















4
0
  2.961e−3
−3.473e−4
  2.525e−5
−1.132e−6
  2.093e−8 


5
0.948
  3.809e−3
−4.033e−4
  2.708e−5
−7.795e−7
−2.784e−8 


15
0.793
−9.040e−4
  4.983e−6
−1.003e−7
  3.506e−3
−3.226e−10


16
1.815
  6.896e−4
  3.467e−6
  1.584e−6
−6.479e−8
  3.664e−9 









In the embodiment, the field curve, the axial aberration and the vertical axis color difference of the wide-angle lens 100 are respectively shown in FIGS. 14, 15, and 16. It can be seen that the field curve is in the range of (−0.05, +0.05), the axial aberration is in the range of (−0.02,+0.02), and the vertical axis color difference is in the range of (−3.5,4-10.0), which indicates that the field curve, the aberration, and the color difference is well corrected in the embodiment.


Table 5 is obtained by summarizing the four embodiments described above, The Table 5 shows the above four embodiments and their corresponding optical characteristics, where the optical characteristic includes system focal length F, aperture number F#, field angle 2θ, and total system length TL, and values corresponding to each previous expression.













TABLE 5





Embodi-
Embodiment
Embodiment
Embodiment
Embodiment


ment
1
2
3
4



















f (mm)
3.31
3.30
3.32
3.32


F#
1.8
1.8
1.8
1.8


2 θ
146°
145°
148°
146°


TL (mm)
27.0
26.4
27.2
27.0


φ27
−0.825
−0.617
−0.687
−0.614


(dN/dT)5 +
−5.4
−5.4
−4.9
−4.9


(dN/dT)6






(dN/dT)2 +
−15.2
−8.7
−8.4
−8.5


(dN/dT)7






φ56
−0.209
−0.430
−0.343
−0.327


φII/φ
0.444
0.615
0.595
0.605


IH/(f *θ)
0.970
0.969
0.962
0.965


T5/T7
1.008
1.785
1.519
1.521


R9/R10
−7.876
−4.085
−2.724
−2.993









According to Table 5, the total optical length of the wide-angle lens 100 is less than 28 mm, the aperture number F# of the wide-angle lens 100 is 1.8, and the field angle 2θ of the wide-angle lens 100 is in the range of 145°˜148°.


Based on above, in specific processes, the wide-angle lens 100 satisfies the following expression: −0.85 <φ27<−0.6, wherein φ2 represents a refractive power of the second lens L2, and φ7 represents a refractive power of the seventh lens L7. The expression indicates that spherical aberration formed by the second lens L2 and the seventh lens L7 cancel each other, which is able to effectively improve an analysis force of the wide-angle lens 100.


Furthermore, the wide-angle lens 100 satisfies the following expression: −5.5<(dN/dT)5+(dN/dT)6<−4,5, wherein (dN/dT)5 represents a temperature coefficient of a refractive index of the fifth lens L5, and (dN/dT)6 represents a temperature coefficient of a refractive index of the sixth lens L6. The expression indicates that the fifth lens L5 and the sixth lens L6 effectively compensate influences of temperature changes on a focal length of the wide-angle lens 100, which further improves stability of the analysis force of the wide-angle lens 100 at different temperatures.


Furthermore, the wide-angle lens 100 satisfies the following expression: −15.5<(dN/dT)2+(dN/dT)7<−8.0, wherein (dN/dT)2 represents a temperature coefficient of refractive index of the second lens L2, and (dN/dT)7 represents a temperature coefficient of a refractive index of the seventh lens L7. When this expression is satisfied, sensitivity of the wide-angle lens 100 to the temperature is effectively reduced, and the stability of the analysis force of the wide-angle lens 100 at different temperatures is further improved.


Furthermore, the wide-angle lens 100 satisfies the following expression: −0.45<φ56<−0.2. wherein φ5 represents a refractive power of the fifth lens L5, and φ6 represents a refractive power of the sixth lens L6. When this expression is satisfied, color difference of the wide-angle lens 100 can be effectively corrected, and the analysis force of the wide-angle lens 100 is further improved.


Furthermore, the wide-angle lens 100 satisfies the following expression: −0.63 <φII/φ<−0.42, wherein φII represents a combined refractive power of the second lens group, and φ represents a refractive power of the wide-angle lens 100. When this expression is satisfied, astigmatism of the wide-angle lens 100 can be effectively corrected, and the analysis force of the wide-angle lens 100 is further improved.


Furthermore, the wide-angle lens satisfies the following expression: 0.95<|IH/(f*θ)|<1, wherein θ represents a maximum half-field angle of the wide-angle lens 100 (representing as radians), IH represents an image height of the wide-angle lens when the half field angle is θ, and f represents an effective focal length of the wide-angle lens 100. This expression indicates radio of an actual image height of the wide-angle lens 100 to an ideal image height of the wide-angle lens.


Furthermore, the wide-angle lens satisfies the following expressions: D1>D2>D3, where D1 represents the maximum diameter of the first lens, D2 represents the maximum diameter of the second lens, D3 represents the maximum diameter of the third lens.


Furthermore, the wide-angle lens satisfies the following expression: 1<T5/T7<2, wherein T5 represents the thickness of the fifth lens, T7 represents the thickness of the seventh lens.


Furthermore, the wide-angle lens satisfies the following expressions: d12>d34>d67, wherein d12 represents the distance between the first lens and the second lens on the optical axis, d34 represents the distance between the third lens and the fourth lens on the optical axis, d67 represents the distance between the sixth lens and the seventh lens on the optical axis.


Furthermore, the wide-angle lens satisfies the following expression: −8<R9/R10<−2, wherein R9 represents a radius of curvature of an object side surface of the fourth lens, Rio represents a radius of curvature of an image side surface of the fourth lens.


Furthermore, the wide-angle lens satisfies the following expression: 0.3<R3/R5<1, wherein R3 represents a radius of curvature of an image side surface of the first lens, R5 represents a radius of curvature of an image side surface of the second lens.


Furthermore, the wide-angle lens satisfies the following expression: 3<R2/R3<5, wherein R2 represents a radius of curvature of an object side surface of the first lens, R3 represents a radius of curvature of an image side surface of the first lens.


According o above structural parameters, the wide-angle lens 100 of the present disclosure at least has following advantages:


(1) The wide-angle lens adopts seven glass lenses, which is clearly imaged in the temperature range of −40° C. to +85° C. and is particularly suitable for camera fields such as motion cameras, vehicle-mounted cameras, which are used in a harsh environment.


(2) The wide-angle lens is clearly imaged through reasonable configuration of focal power combinations between the lenses, which can match with imaging chips with more than eight million pixels.


(3) A field angle of the wide-angle lens can reach 146 degrees, distortion of f-θ is effectively corrected, and the distortion of f-θ is controlled to be less than 5%. Thus, requirements of a large field angle are satisfied.


(4) An aperture number of the wide-angle lens is 1.8, which satisfies an imaging requirement of a darker environment.


The above-mentioned embodiments merely illustrate several embodiments of the present disclosure, and the description thereof is specific and detailed, which cannot to be understood as a limit to the disclosed embodiments. It should be noted that a number of variations and modifications may be made by person skilled in the art without departing from the spirit and scope of the present disclosure. The scope of the present disclosure should be determined by the appended claims.

Claims
  • 1. A wide-angle lens, from an object side to an imaging surface, comprising a first lens group having a negative focal power, a second lens group having a positive focal power, and an aperture stop disposed between the first lens group and the second lens group; wherein the first lens group, from the object side to the imaging surface, sequentially comprises a meniscus-shaped first lens having a negative focal power, a second lens having a negative focal power, and a third lens having a positive focal power; a concave surface of the first lens faces the imaging surface, and a concave surface of the second lens faces the imaging surfacethe second lens group, from the object side to the imaging surface, sequentially comprises a fourth lens having a positive focal power, a fifth lens having a positive focal power, a sixth lens having a negative focal power, and a seventh lens having a positive focal power; the fourth lens, the fifth lens, and the seventh lens are biconvex lenses; and the sixth lens is a biconcave lens;the fifth lens and the sixth lens cemented a cemented lens; andthe first lens, the third lens, the fourth lens, the fifth lens, and the sixth lens are glass spherical lenses; the second lens and the seventh lens are glass aspherical lenses; and optical center bits of the lenses in the first lens group and the second lens group are located on a same straight linewherein the wide-angle lens satisfies the following expression: −0.85 <φ2/φ7<−0.6; wherein φ2 represents a refractive power of the second lens, and φ7 represents a refractive power of the seventh lens.
  • 2. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: −5.5×10−6/K <(dN/dT)5+(dN/dT)6<−4.5×10−6/K; wherein (dN/dT)5 represents a temperature coefficient of a refractive index of the fifth lens, and (dN/dT)6 represents a temperature coefficient of a refractive index of the sixth lens.
  • 3. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: −15.5×10−6/K <(dN/dT)2+(dN/dT)7<−8.0×10−6/K; wherein (dN/dT)2 represents a temperature coefficient of a refractive index of the second lens, and (dN/dT)7 represents a temperature coefficient of a refractive index of the seventh lens.
  • 4. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: −0.45<φ5/φ6−0.2; wherein φ5 represents a refractive power of the fifth lens, and φ6 represents a refractive power of the sixth lens.
  • 5. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: 0.63<φII/φ<0.42; wherein φII represents a combined refractive power of the second lens group, and φ represents a refractive power of the wide-angle lens.
  • 6. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: 0.95 <|IH/(f*θ)|<1; wherein θ represents a maximum half-field angle of the wide-angle lens, IH represents an image height of the wide-angle lens when the half field angle is θ, and f represents an effective focal length of the wide-angle lens.
  • 7. The wide-angle lens according to claim 1, wherein surface shapes of the second lens and the seventh lens satisfy the following formula:
  • 8. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expressions: D1>D2>D3, where D1 represents the maximum diameter of the first lens, D2 represents the maximum diameter of the second lens, D3 represents the maximum diameter of the third lens.
  • 9. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: 1<T5/T7<2, wherein T5 represents the thickness of the fifth lens, T7 represents the thickness of the seventh lens.
  • 10. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expressions: d12>d34>d67, wherein d12 represents the distance between the first lens and the second lens on the optical axis, d34 represents the distance between the third lens and the fourth lens on the optical axis, d67 represents the distance between the sixth lens and the seventh lens on the optical axis.
  • 11. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: −8<R9/R10<−2, wherein R9 represents a radius of curvature of an object side surface of the fourth lens, R10 represents a radius of curvature of an image side surface of the fourth lens.
  • 12. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: 0.3<R3 /R5<1, wherein R3 represents a radius of curvature of an image side surface of the first lens, R5 represents a radius of curvature of an image side surface of the second lens.
  • 13. The wide-angle lens according to claim 1, wherein the wide-angle lens satisfies the following expression: 3<R2/R3<5, wherein R2 represents a radius of curvature of an object side surface of the first lens, R3 represents a radius of curvature of an image side surface of the first lens.
  • 14. A wide-angle lens, from an object side to an imaging surface, comprising a first lens group having a negative focal power, a second lens group having a positive focal power, and an aperture stop disposed between the first lens group and the second lens group; wherein the first lens group, from the object side to the imaging surface, sequentially comprises a meniscus-shaped first lens having a negative focal power, a second lens having a negative focal power, and a third lens having a positive focal power; a concave surface of the first lens faces the imaging surface, and a concave surface of the second lens faces the imaging surfacethe second lens group, from the object side to the imaging surface, sequentially comprises a fourth lens having a positive focal power, a fifth lens having a positive focal power, a sixth lens having a negative focal power, and a seventh lens having a positive focal power; the fourth lens, the fifth lens, and the seventh lens are biconvex lenses; and the sixth lens is a biconcave lens;the fifth lens and the sixth lens cemented a cemented lens; and
  • 15. A wide-angle lens, from an object side to an imaging surface, comprising a first lens group having a negative focal power, a second lens group having a positive focal power, and an aperture stop disposed between the first lens group and the second lens group; wherein the first lens group, from the object side to the imaging surface, sequentially comprises a meniscus-shaped first lens having a negative focal power, a second lens having a negative focal power, and a third lens having a positive focal power; a concave surface of the first lens faces the imaging surface, and a concave surface of the second lens faces the imaging surfacethe second lens group, from the object side to the imaging surface, sequentially comprises a fourth lens having a positive focal power, a fifth lens having a positive focal power, a sixth lens having a negative focal power, and a seventh lens having a positive focal power; the fourth lens, the fifth lens, and the seventh lens are biconvex lenses; and the sixth lens is a biconcave lens;the fifth lens and the sixth lens cemented a cemented lens; and
Priority Claims (1)
Number Date Country Kind
201810549888.2 May 2018 CN national
CROSS REFERENCE TO RELATED APPLICATION(S)

This application is a continuation of International Application No. PCT/CN2019/085183, filed on Apr. 30, 2019, which claims the priority benefit of a Chinese Patent Application No. 2018105498882, filed on May 31, 2018. The entireties of the above-mentioned applications are hereby incorporated by reference herein.

US Referenced Citations (4)
Number Name Date Kind
6014268 Yahagi Jan 2000 A
20070139787 Kim Jun 2007 A1
20150260968 Ohashi Sep 2015 A1
20160363740 Gong Dec 2016 A1
Related Publications (1)
Number Date Country
20200363609 A1 Nov 2020 US
Continuations (1)
Number Date Country
Parent PCT/CN2019/085183 Apr 2019 US
Child 16986211 US