Abstract:
A telephoto zoom lens having four lens groups of which the 1st, counting from the front, has a positive refractive power, the 2nd has a negative refractive power, the 3rd has a positive refractive power and the 4th has a positive refractive power. The 1st, 2nd and 3rd lens groups form a varifocal section, and the 1st and 2nd lens groups axially move in opposite directions to each other when zooming. The amounts of movement of the 1st and 2nd lens groups relative to each other are thus controlled to achieve a shortening of the total length of the lens system.

Description:
This is a continuation of application Ser. No. 652,421, now abandoned filed Sept. 19, 1984, which was a continuation of application Ser. No. 373,642, filed Apr. 30, 1982, now abandoned. 
    
    
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     This invention relates to telephoto zoom lenses and, more particularly, to telephoto zoom lenses having four lens groups of which the first three counting from the front are movable to effect a change in image magnification, with the total length of the lens system being shortened. 
     2. Description of the Prior Art 
     In the past, as one type of zoom lens, there has been known a lens system consisting of four lens groups having positive, negative, positive and positive refractive powers arranged in this order from the front. In such zoom lens the 2nd lens group is moved axially to effect variation in the focal length, while the image shift compensation is effected by the axial movement of the 3rd lens group in a path concave toward the front. However, generally in this type of zoom lens, an increase in the zoom ratio or the relative aperture calls for a rapid increase of the total length of the lens system or the diameter of the front lens members. Further, to maintain the constant total length of the lens system during zooming, a large limitation must be given to the ratio of the distance from the front vertex to the focal plane to the longest focal length, that is, the telephoto ratio. Also, to suppress this to a minimum, the refractive power of each of the lens group in the varifocal section must be strengthened, thereby producing disadvantages that the necessary number of constituent lens elements is increased and good correction of principal aberrations becomes difficult to perform. On the other hand, it is known to provide zoom lenses of which the varifocal section includes three or more lens groups as in Japanese Laid-Open Patent No. Sho 53-34539, and U.S. Pat. Nos. 4,172,635, 4,196,969 and 4,240,760. These zoom lenses must however be provided with their operating mechanisms of complex structure, and such configuration cannot always be said to be suitable for use in the telephoto type zoom lens. 
     SUMMARY OF THE INVENTION 
     It is an object of the present invention to provide a telephoto zoom lens of very simple configuration in the expanded form of the conventional two-movable component zoom type that three lens groups are axially moved, while still permitting the total length of the lens system to be shortened when in the shortest settings. 
     A feature of lens construction of the telephoto zoom lens which is considered to be characteristic of the present invention is that a 1st lens group of positive power, a 2nd lens group of negative power, a 3rd lens group of positive power and a 4th lens group of positive power are arranged in this order from the front and the 1st, 2nd and 3rd lens groups constitute a varifocal section, wherein the 1st and 2nd lens groups are axially moved in opposite directions to each other while the amounts of movement of the 1st and 2nd lens groups in differential relation are controlled, thus accomplishing the object of the present invention. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIGS. 1, 2 and 3 are lens block diagrams of embodiments 1, 2, and 3 of telephoto zoom lenses according to the present invention respectively. 
     FIGS. 4-a-1 to 3, 4-b-1 to 3 and 4-c-1 to 3 are aberration curves of the lens of FIG. 1. 
     FIGS. 5-a-1 to 3, 5-b-1 to 3 and 5-c-1 to 3 are aberration curves of the lens of FIG. 2. 
     FIGS. 6-a-1 to 3, 6-b-1 to 3 and 6-c-1 to 3 are aberration curves of the lens of FIG. 3. 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     The zoom lens of the invention will be better understood from the following descriptions made with reference to the drawings. The zoom lens comprises, from front to rear, a 1st lens group I of positive power, a 2nd lens group II of negative power, and a 3rd lens group III of positive power and further includes a 4th lens group IV for forming an image of an object. Letting fI, fII, fIII and fIV denote the focal lengths of the lens groups I to IV respectively, e&#39; 1  the interval between the principal planes of the 1st and 2nd lens groups I and II when in the shortest focal length position, e&#39; 2  the interval between the principal planes of the 2nd and 3rd lens groups II and III, ξ, η and γ the amounts of movement of the 1st, 2nd and 3rd lens groups I, II and III by taking the positions of the 1st, 2nd and 3rd lens groups I, II and III when in the shortest focal length setting as respective start points with a position sign being given when measured along the optical axis from the front to rear, ξa and ηa the total movements of the 1st and 2nd lens groups I and II from the shortest to the longest focal length position, Z the zoom ratio, and Ka(=ξa/η/a) the ratio of the total movement of the 1st lens group I to that of the 2nd lens group II, we have the amount of movement γ of the 3rd lens group III as a solution of the following quadratic equation: ##EQU1## 
     In the present invention, to vary the focal length of the engtire lens system, the 1st and 2nd lens groups I and II are made to be axially movable in opposite directions to each other. In this case, as the 1st lens group I is pulled out forward by the actuator, the 2nd lens group II has to move in driven connection thereto, so that when the amount of movement of the 2nd lens group II is far larger than that of movement of the 1st lens group I, an unduly large stress is put on the operating mechanism. Though this drawback can be overcome by using an alternate arrangement where the 2nd lens group II is moved by the actuator, while the 1st lens group is made to follow it up, it is found that since the amount of movement ξ of the 1st lens group I is small, the advantage of the invention is reduced, being almost equal to that expected from the conventional type of zoom lens in which only one or the 2nd lens group II is moved to effect a change in focal length. 
     On the other hand, when the amount of movement ξ on the 1st lens group I is very large, the total length of the lens system when in telephoto settings becomes longer so that though the aberration correction becomes easy, the diameter of the front lens members must be increased to an objectionable point. In the present invention, a good result is obtained by satisfying the following conditions: 
     
         -5.1&lt;Ka&lt;-0.4                                               (1) 
    
     where Ka is the ratio of the total movement of the 1st lens group I to that of the 2nd lens group II. 
     Also in the present invention, with the 1st and 2nd lens groups made to move on the common optical axis in opposite directions to each other rectilinearly so that the on-axis rays emerge out of the 3rd lens group III almost in parallelism, it is made possible to eliminate variation with zooming of aberrations by simple techniques and also to minimize the zonal spherical aberration. It is to be noted that the 1st and 2nd lens groups I and II may be moved non-rectilinearly. 
     Further, for a lens system in which the 3rd lens group III takes the same position when in the shortest and longest focal length settings we have the following formula: 
     
         p.sup.2 =-Z×fII.sup.2 (K-1) 
    
     
         ηa(1-K)=p×(1-1/Z) 
    
     where K is the ratio of the amount of movement ξ of the 1st lens group I to that of movement η of the 2nd lens group II. 
     At this time, the focal length fIII of the 3rd lens group III is determined by: 
     
         fIII=e&#39;.sub.2 -[fII·(fI-e&#39;.sub.1)]/p 
    
     imparting of such perfect reciprocating motion to the 3rd lens group III produces an advantage that, since the 3rd lens group III lies at the same point in position for both of the shortest and longest focal lengths of the entire lens system and contributes equal aberrations to the system, all that is needed to be taken into account is the stability of aberration correction in the intermediate focal length region. It is therefore made possible to construct even the 3rd lens group in the form of a singlet lens. 
     In order that the ratio K obtained by solving the above equations satisfies the before-mentioned condition (1), it is preferred to set forth the following conditions: 
     
         1.4&lt;(fI+fII-e&#39;.sub.1).sup.2 /(Z·fII.sup.2)&lt;6.1    (2) 
    
     
         1.4&lt;(fI+fII-e&#39;.sub.1)(1-1/Z)/ηa&lt;6.1                    (3) 
    
     When the lower limits of conditions (2) and (3) are exceeded, as the amount of movement of the 1st lens group I becomes relatively small to the amount of movement of the 2nd lens group II, the refractive power of the 1st lens group I must be strengthened. If the number of lens elements constituting the 1st lens group is not increased, it becomes difficult to remove the variation of aberrations with focusing to shorter object distances. Further, the amount of movement of the 2nd lens group II increases. To avoid this, by strengthening the refractive power of the 2nd lens group II, the refractive power of each of the other lens groups must be necessarily increased, thereby giving a disadvantage that the range of variation of spherical aberration with zooming is increased. On the other hand, when the upper limits of conditions (2) and (3), the amount of movement of the 1st lens group I becomes relatively large to the amount of movement of the 2nd lens group II. This calls for an increase in the total length of the lens system when in the longest focal length positions and an increase in the diameter of the front lens members. In addition thereto, it becomes difficult to remove the positive distortion in the long focal length positions. 
     Therefore, the choice of a refractive power distribution satisfying conditions (2) and (3) makes it possible to reduce the increase of the Petzval sum in a negative sense resulting from the limitation of the telephoto ratio to a minimum, for the total length of the lens system would be otherwise elongated in the long focal length positions, and makes it possible to eliminate variation of the spherical aberration resulting from the increase in the refractive power of each of the lens groups. Moreover, since the total length of the lens system in the short focal length positions is short, the burden of carrying about the lens in attachment to the camera body can be considerably reduced. 
     Next, the numerical data for embodiments of the invention satisfying the above-cited conditions are given. The embodiments are zoom lenses having a focal length range of 103 to 197 mm with an F-number of 1:4.5. In the following tables, Ri is the radius of curvature of the i-th lens surface counting from the front, Di is the i-th axial lens thickness or air separation counting from the front, and Ni and νi are respectively the refractive index of Abbe number for spectral d-line of the glass from which the i-th lens element counting from the front is made up. 
     
         ______________________________________Example 1F=103-197 FNo.=1:4.5 2ω=24-12______________________________________fI=94.81R1=109.46   D1=2.30     N1=1.80518                                 ν1=25.4R2=59.49    D2=7.00     N2=1.61800                                 ν2=63.4I    R3=-1037.84 D3=0.15R4=110.78   D4=4.00     N3=1.61800                                 ν3=63.4R5=-1888.22 D5=VariablefII=-30.00R6=-256.99  D6=2.00     N4=1.77250                                 ν4=49.6R7=113.61   D7=5.54R8=-121.66  D8=3.90     N5=1.84666                                 ν5=23.9II   R9=-30.80   D9=1.50     N6=1.69680                                 ν6=55.5R10=234.21  D10=1.86R11=-55.78  D11=1.36    N7=1.69680                                 ν7=55.5R12=199.81  D12=VariablefIII=73.71R13=126.42  D13=6.80    N8=1.65830                                 ν8=53.4R14=-28.53  D14=1.50    N9=1.84666                                 ν9=23.9III  R15=-55.96  D15=VariableR16=0.0     D16=1.50fIV=135.63R17=49.80   D17=7.00    N10=1.58904                                 ν10=53.2R18=-87.10  D18=1.90    N11=1.84100                                 ν11=43.2R19=3540.44 D19=51.02IV   R20=86.07   D20=4.00    N12=1.57845                                 ν12=41.5R21=-353.40 D21=5.98R22=-34.68  D22=2.00    N13=1.72000                                 ν13=46.0R23=-113.86D/F      103.0         150.35  197.0D5       1.97          17.97   26.21D12      17.80         9.66    1.64D15      4.00          1.47    4.00(fI+fII-e&#39;.sub.1).sup.2 /(ZfII.sup.2)=1.53 -(fI+fII-e&#39;.sub.1)(1-1/Z)/ηa=1.5______________________________________ 
    
     
         ______________________________________Example 2F=103-197 FNo.=1:4.5 2ω=24-12______________________________________fI=120.68R1=75.54    D1=2.20     N1=1.80518                                 ν1=25.4R2=48.97    D2=7.00     N2=1.53996                                 ν2=59.5I    R3=-384.66  D3=0.15R4=157.01   D4=3.00     N3=1.51633                                 ν3=64.1R5=315.56   D5=VariablefII=-36.0R6=-360.24  D6=1.60     N4=1.71285                                 ν4=43.2R7=44.79    D7=4.13II   R8=-42.08   D8=1.60     N5=1.74320                                 ν5=49.3R9=39.05    D9=5.00     N6=1.80518                                 ν6=25.4R10=-131.66 D10=VariablefIII=81.35R11=168.47  D11=6.80    N7=1.62374                                 ν7=47.1R12=-30.21  D12=1.50    N8=1.80518                                 ν8=25.4III  R13=-54.76  D13=VariableR14=0.0     D14=1.50fIV=144.04R15=53.59   D15=8.00    N9=1.63930                                 ν9=44.9R16=-81.31  D16=1.90    N10=1.84666                                 ν10=23.9R17=904.24  D17=70.65IV   R18=-25.90  D18=1.78    N11=1.69350                                 ν11=53.2R19=- 38.22 D19=0.15R20=61.74   D20=3.60    N12=1.67270                                 ν12=32.1R21=82.98D/F      103.0         150.35  197.0D5       1.63          25.14   37.26D10      16.56         8.58    0.72D13      4.00          1.52    4.00(fI+fII-e&#39;.sub.1).sup.2 /(ZfII.sup.2)=2.25(fI+fII-e&#39;.sub.1)(1-1/Z)/ηa=2.25______________________________________ 
    
     
         ______________________________________Example 3F=103-197 FNo.=1:4.5 2ω=24-12______________________________________fI=184.50R1=122.19    D1=2.50  N1=1.76182                               ν1=26.6R2=61.12     D2=1.20I    R3=62.09     D3=9.00  N2=1.60729                               ν2=49.2R4=-335.00   D4=VariablefII=-40.0R5=-112.40   D5=1.60  N3=1.71300                               ν3=53.8R6=111.92    D6=4.70II   R7=-89.96    D7=1.60  N4=1.69680                               ν4=55.5R8=32.55     D8=4.00  N5=1.80518                               ν5=25.4R9=118.98    D9=VariablefIII=73.81R10=184.12   D10=6.80  N6=1.58904                               ν6=53.2R11=-28.94   D11=1.50  N7=1.80518                               ν7=25.4III  R12=-44.98   D12=VariableR13=0.0      D13=1.50fIV=139.58R14=41.40    D14=7.00  N8=1.61117                               ν8=55.9R15=-226.83  D15=0.90R16=-108.81  D16=1.90  N9=1.84666                               ν9=23.9R17=978.60   D17=65.28IV   R18=-24.67   D18=1.78  N10=1.69680                               ν10=55.5R19= -47.73  D19=0.15R20=91.58    D20=3.60  N11=1.59270                               ν11=35.3R21=-14415.58D/F      103.0         150.35  197.0D4       1.43          44.10   66.09D9       12.60         7.17    1.83D12      4.00          2.32    4.00(fI+fII-e&#39;.sub.1).sup.2 /(ZfII.sup.2)=6.0(fI+fII-e&#39;.sub.1)(1-1/Z)/ηa=6.0______________________________________