Distance measurement apparatus for camera

Abstract: According to the invention, a distance measurement apparatus for a camera is disclosed. In this apparatus, a plurality of light-emitting elements (6) are arranged at dif­ ferent positions in a direction perpendicular to a base line and an optical axis of projected light. A driver (7) causes the light-emitting elements (6) to selectively emit near-distance measurement light and far-distance measure­ ment light having a higher intensity than that of the near-distance measurement light. When an amount of light reflected by an object cannot reach a predetermined value necessary for distance measurement upon emission of a light-emitting element (6) selected by the driver (7), a microcom­ puter (11) controls an operation of the driver (7) so as to cause another light-emitting element (6) to emit light. The near- or far-distance measurement light reflected by the object is received so as to measure a distance (R) to the object.

Description: BACKGROUND OF THE INVENTION The present invention relates to an active type distance measurement apparatus for a camera. A variety of methods are employed for an automatic focusing (auto-focus) function of a camera. One of these methods is a method wherein a distance to an object is measured using an active type distance measurement apparatus, and a photographing lens is moved in accordance with the measured distance. Fig. 10 is a view for explaining the principle of the active measuring method. In Fig. 10, reference numeral 1 denotes a distance measurement light projecting lens; 2, a distance measurement light receiving lens; 3, an infrared LED; 4, an object; and 5, a PSD (Position Sensitive Device) as a light-receiving element. The PSD 5 is a light-receiving element which can provide two current outputs I₁ and I₂ as shown in Fig. 11 when it receives an LED image on its element surface. If a distance from the center of the element surface to an LED image P is given as x , the following relationship is established between the distance x and the currents I₁ and I₂: x = K·ℓ n (I₁/I₂) (1) K: constant Assume that an image of an object which is located at an infinity point is formed at the center of the PSD 5, and a photographing lens (not shown) is set to be focused at the infinity point. When the object 4 separated from a camera by a finite distance or less is then subjected to distance measurement, a projected spot image is focused on the PSD 5 separated from the center by the distance x . In this case, the following relationship is established between a distance R to the object 4 and the distance x : where B is a distance (base length) between the light projecting lens 1 and the light receiving lens 2, and f₂ is a focal length of the light receiving lens 2. If a position on an optical axis of the photographing lens which can be focused for the object distance R is given as y to have an origin on the optical axis when the photographing lens is focused at the infinity point, y represents a defocusing amount, and R is represented as follows in accordance with the relation (1/R) + {1/(f + y) } = (1/f) : f: focal length of photographing lens Therefore, from equations (1) to (3), y can be calculated as follows: More specifically, calculation is made using the current outputs I₁ and I₂ of the PSD 5 to obtain x , and x is substituted into equation (4) to obtain the defocusing amount y . In recent auto-focus cameras, a variety of attempts are made to extend a possible photographing range, and a strong demand has arisen for proximity photographing. However, in the conventional active method, as the object 4 comes closer, the LED image P moving along the PSD 5 is moved to the left in Fig. 11. As the displacement of the LED image P comes closer to half a length L of the PSD 5 (i.e., L/2), the LED image P begins to fall outside the PSD 5. The LED image P falls outside the PSD 5 finally and precise distance measurement cannot be performed. In this case, the length L of the PSD 5 may be prolonged. However, the length L of the PSD 5 is limited in association with the installation space in a camera and cost. If light reflected by a near object 4 can be received by the PSD 5 in a predetermined light emission amount of the LED 3, as the object 4 comes closer, the reflection light becomes stronger, and the output from the PSD 5 is increased and saturated over the dynamic range. Thus, accurate distance measurement cannot be performed either. In this case, if the output from the LED 3 is increased in order to improve far-distance measurement performance, the near-distance measurement becomes more difficult. If the area of an LED chip is simply increased to increase the output from the LED 3, the size of the projected LED image is increased, and a far-distance measurement error may occur. For example, in Fig. 12, assume that an object is located at a position C. If a projected LED image from the LED 3 is radiated on the entire object and is reflected thereby, the center of gravity of the received LED image on the PSD 5 coincides with a point P. However, when only a portion of the projected LED image (hatched portion in Fig. 12) is radiated on the object and is reflected thereby, the center of gravity of the received LED image coincides with a point Q. For this reason, although the object is located at the position C, the positions of the received LED images on the PSD 5 are different, and different distance measurement results are obtained, resulting in a distance measurement error. As described above, in the conventional distance measurement apparatus, it is difficult to accurately perform both far- and near-distance measurements. Accordingly, an object of the present invention is to provide an active distance measurement apparatus which can accurately perform both far and near distance measurements. Document US-A-4688919 describes a distance measurement apparatus for a camera, comprising: at least first and second light-emitting elements disposed along a base line perpendicular to the optical axis of a camera lens and disposed to emit light beams towards an object to be photographed; light receiving means extended along said base line to receive a said light beam reflected by said object and to provide an electric signal representative of the position along said receiving means at which said received light beam is incident; and arithmetic means for calculating the distance to said object in accordance with said electric signal. The measurement principles discussed above in relation to Figures 10 to 12 herein can be represented by Document US-A-4688919. The present invention is characterised by: drive means operable to cause said first light-emitting element to selectively emit a first light beam and said second light-emitting element to selectively emit a second light beam, said first light beam being of higher intensity than said second light beam and said first element being disposed closer than said second element to said light receiving means; control means for controlling operation of said drive means in accordance with the intensity of the light beam received by said light receiving means to select said first element when said received intensity is low and said second element when said received intensity is relatively high, whereby said first element is used for measurement of far distances and said second element for relatively near distances; and correction means for providing a correction signal effective to correct the distance calculated by said arithmetic means in accordance with the element currently selected by said drive means. An embodiment of the invention will now be described, by way of Example, with reference to the accompanying drawings, in which: Fig. 1 is a block diagram showing a distance measurement apparatus for a camera; Fig. 2 is a front view of an infrared LED used in the embodiment shown in Fig. 1; Fig. 3 is a flow chart for explaining a distance measurement operation of the apparatus shown in Fig. 1; Figs. 4A to 4C are views showing other arrangements of a light-emitting portion of the infrared LED; Fig. 5 is a block diagram showing an embodiment of the present invention; Fig. 6 is a front view of an infrared LED used in the embodiment shown in Fig. 5; Fig. 7 is a view for explaining a correction amount of a light spot position of a PSD; Fig. 8 is a flow chart for explaining the operation of the embodiment shown in Fig. 5; Figs. 9A to 9C are views showing other arrangements of a light-emitting portion of the infrared LED used in the embodiment shown in Fig. 5; Fig. 10 is a view for explaining the principle of an active distance measurement method; Fig. 11 is a view for explaining a PSD; and Fig. 12 is a view for explaining a distance measurement error upon far-distance measurement. Fig. 1 is a block diagram showing a distance measurement apparatus for a camera, and the same reference numerals in Fig. 1 denote the same parts as in Fig. 10. In Fig. 1, reference numeral 6 denotes an infrared LED serving as a light-emitting element. As shown in Fig. 2, the LED 6 has two light-emitting portions L₁ and L₂ at different positions in a direction perpendicular to a base line A (a line connecting a PSD 5 and the LED 6). The light-emitting portions L₁ and L₂ have an identical light-emitting intensity. In a far-distance measurement mode, both the light-emitting portions L₁ and L₂ emit light. In a near-distance measurement mode, only the light-emitting portion L₂ emits light. Reference numeral 7 denotes a driver for supplying a predetermined drive pulse signal to the LED 6 so as to cause the light-emitting portions L₁ and L₂ of the LED 6 to selectively emit light. An arithmetic processor 8 checks if a signal output from the PSD 5 falls within its dynamic range. If the signal output falls within the dynamic range, the processor 8 calculates a distance x based on equation (1) described above. If the signal output from the PSD 5 falls outside its dynamic range, the processor 8 outputs a re-emission signal to a microcomputer 11. Whether or not the signal output from the PSD 5 falls within its dynamic range is determined as follows. For example, the output currents I₁ and I₂ from the PSD 5 are converted to voltage values V₁ and V₂ by I-V converters, and the voltage values V₁ and V₂ are compared with reference voltages by comparators. For example, if the voltage value V₁ is larger than a predetermined lower-limit value a and the voltage value V₂ is smaller than a predetermined upper-limit value b (a < V₁, V₂ < b), or when the sum (V₁ + V₂) of the voltage values V₁ and V₂ is larger than a predetermined lower-limit value c and is smaller than a predetermined upper-limit value d (c < V₁ + V₂ < d), it is determined that the signal output from the PSD 5 is at a level necessary for distance measurement. The calculation result x from the arithmetic processor 8 is A/D-converted to digital data by an A/D converter 9, and the digital data is supplied tc a microcomputer 11. The microcomputer 11 calculates a defocusing amount y of a photographing lens (not shown) using the distance x based on the equation (4) described above, and drives a lens actuator 10 in accordance with the calculated value y . The photographing lens is moved by the defocusing amount y by the lens actuator 10, and is stopped at an in-focus position. Note that reference symbols S₁ and S₂ denote switches which are turned on upon operation of a release button. The switch S₁ is turned on when the release button is lightly depressed by the first stroke, and the switch S₂ is turned on when the release button is depressed further deeply by the second stroke. The distance measurement operation will be described with reference to the flow chart shown in Fig. 3. When a photographer lightly depresses the release button by the first stroke, the switch S₁ is turned on (F-1), and a light emission instruction is output from the microcomputer 11 to the driver 7. Thus, the drive pulse signal is supplied from the driver 7 to the light emitting portions L₁ and L₂ of the LED 6, thereby emitting infrared light pulses for far-distance measurement (F-2). The infrared light pulses are projected forward through the light projecting lens 1, are then reflected by the object 4, and are received on the PSD 5 through the light receiving lens 2. The currents I₁ and I₂ are output from the PSD 5 to the arithmetic processor 8. The arithmetic processor 8 checks if the output currents I₁ and I₂ are at a minimum level or higher necessary for calculation (F-3). If YES in step F-3, it is checked if the outputs from the PSD 5 are saturated (F-4). In these steps F-3 and F-4, it can be determined if the outputs from the PSD 5 fall within the dynamic range. If the outputs from the PSD 5 fall within the dynamic range, the arithmetic processor 8 calculates the distance x based on the above-mentioned equation (1) (F-5), and the distance x is A/D-converted to digital data by the A/D converter 9. The digital data is then read by the microcomputer 11 (F-6). The microcomputer 11 calculates the defocusing amount y based on equation (4) (F-7). As described above, since both the light-emitting portions L₁ and L₂ of the LED 6 are operated to output the infrared light pulses for far-distance measurement, a distance to a far-distance object can be measured. Since the light-emitting portions L₁ and L₂ are arranged in a direction perpendicular to the base line A, as described above, the width of the spot light in the direction of the base line can be reduced as compared to cases wherein the same amount of light is projected using a square LED having the same area as the total area of the portions L₁ and L₂ or wherein the light is projected from two LEDs arrayed in the direction of the base line (see Fig. 12). Therefore, a distance measurement error can be eliminated, and accurate far-distance measurement can be performed. In this case, another arrangement may be proposed in order to increase a light-emitting intensity. That is, two LEDs are arrayed in the direction of the base line for far-distance measurement. However, with this arrangement, since the centers of gravity of LED images on the PSD are different from each other, the distance measurement result must be corrected. If the light-emitting portions L₁ and L₂ of the LED 6 are arrayed in a direction perpendicular to the base line A, the center of gravity of the spot image is not changed, and no correction is required. If the outputs from the PSD 5 are saturated (F-4), the arithmetic processor 8 outputs a re-emission signal to the microcomputer 11. In response to this, the microcomputer 11 outputs a re-emission instruction to the driver 7. The driver 7 causes the light-emitting portion L₂ to output infrared light pulses for near-distance measurement (F-8). The reason why the outputs from the PSD 5 are saturated is that the object 4 is too close and light reflected thereby is too strong. Thus, if only the light-emitting portion L₂ emits light, the light reflected by the object 4 becomes weak, and the outputs from the PSD 5 are not saturated but can be precise values. The arithmetic processor 8 checks if the outputs from the PSD 5 are sufficient upon emission of the light-emitting portion L₂ (F-9). If YES in step F-9, it is checked if the outputs from the PSD 5 are saturated (F-10). If NO in step F-10, the distance x is calculated based on the output currents (F-5), and the calculated distance x is converted to digital data. The digital data is read by the microcomputer 11 (F-6). Then, the microcomputer 11 calculates the defocusing amount y (F-7). If the outputs from the PSD 5 are not sufficient (F-3 or F-9), or if the outputs therefrom are saturated (F-10), it is determined that the object distance is the farthest distance (e.g., infinity) or closest distance (e.g., 50 cm or less). Therefore, the defocusing amount y is set to 0 or ymax. More specifically, if both the outputs from the PSD 5 are not sufficient upon emission of the light-emitting portions L₁ and L₂, the object distance is determined to be an infinity, and the amount y is set to be 0 (F-11). However, if the outputs from the PSD 5 are saturated, the object distance is determined to be shorter than the closest distance, and the amount y is set to be ymax (F-12). When the distance measurement operation is completed as described above and the release button is depressed deeper, the switch S₂ is turned on (F-13). Thereby, the photographing lens is moved by the defocusing amount y calculated previously (F-14). Then, a shutter is driven (F-15), thus completing a photographing operation. In the above embodiment, the light-emitting portions L₁ and L₂ of the LED 6 have a rectangular shape of an identical size, as shown in Fig. 2. However, the present invention is not limited to this. For example, the light-emitting portions L₁ and L₂ may have shapes as shown in Figs. 4A to 4C. In this case, the light-emitting portions preferably have a small width in the direction of the base line A, and are preferably elongated in a direction perpendicular to the base line A in order to reduce a distance measurement error. In the above arrangement, both the light-emitting portions L₁ and L₂ emit light for far-distance measurement. Instead, the light emission intensity of the light-emitting portion L₁ may be increased for far-distance measurement, and the light-emitting portion L₂ may be operated for near-distance measurement. The light-emitting element has two light-emitting portions. However, a larger number of light-emitting portions or light-emitting elements may be employed as long as a camera space or optical system design allows. In this manner, more accurate distance measurement can be achieved. In the above embodiment, a light-emitting circuit is controlled such that light for far-distance measurement is emitted first, and then, light for near-distance measurement is emitted. However, the light-emission order may be reversed as needed. According to the present arrangement as described above, a plurality of light-emitting elements are arranged at different positions in a direction perpendicular to the base line and the optical axis of projected light, and are selectively emitted so as to selectively emit near-distance measurement light and far-distance measurement light, thereby measuring a distance to an object. Thus, far-distance measurement is performed using projected light having a high intensity and a small width in the direction of the base line, and near-distance measurement is performed using a low intensity. Thus, both far and near distances can be accurately measured. Fig. 5 shows an embodiment of the present invention. The same reference numerals in Fig. 5 denote the same parts as in Fig. 1, and a detailed description thereof will be omitted. In Fig. 5, reference numeral 12 denotes an infrared LED serving as a light-emitting element. As shown in Fig. 6, the LED 12 has two light-emitting portions L₃ and L₄ at different positions in a direction of a base line A. The light-emitting portion L₃ is used for far-distance measurement, and the light-emitting portion L₄ is used for near-distance measurement. The light emission intensity of the light-emitting portion L₃ is higher than that of the light-emitting portion L₄. The light-emitting portion L₄ is arranged at a position opposite to a PSD 5. Reference numeral 13 denotes a driver for selectively causing the light-emitting portions L₃ and L₄ to emit light; 14, a semifixed resistor for setting a correction amount Δx for correcting a calculation result x of an arithmetic processor 8; and 15, an A/D converter for A/D-converting the correction amount (voltage value) set by the semifixed resistor 14 into digital data and supplying it to a microcomputer 11. In this embodiment, the light-emitting portions L₃ and L₄ are arranged at an interval in the direction of base line. For this reason, an LED image formed upon emission of the light-emitting portion L₄ is located on the PSD 5 nearer the LED 12 than an LED image formed on the PSD 5 upon emission of the light-emitting portion L₃. When the light-emitting portion L₄ emits light, the calculation result x must be corrected by a predetermined correction amount Δx. The correction will be described with reference to Fig. 7. Assume that a distance to a wall W separated from a light projecting lens 1 by R. Light emitted from the light-emitting portion L₃ is reflected at a point W₃ of the wall W, and is focused at a point P₃ on the PSD 5. However, light emitted from the light-emitting portion L₄ is reflected at a point W₄, and is focused on a point P₄. When the light-emitting portion L₄ is used, correction can be made such that the point P₄ coincides with the point P₃. A distance between the points P₄ and P₃ is given as a correction amount Δx. When the light-emitting portion L₄ is used, Δx can be added to the light spot position of the PSD 5, thus achieving correction. If a distance between the light-emitting portions L₃ and L₄ is given as ΔL, and focal lengths of the light projecting lens 1 and light receiving lens 2 are respectively given as f₁ and f₂, and a distance between the points W₃ and W₄ is given as U, U is expressed by: If a distance from the center of the PSD 5 to the point P₃ is given as x , and a distance to the point P₄ is given as α, since (U - B) : R = α : f₂, α is given by: therefore, In this manner, the correction amount Δx can be calculated in advance using parameters f₁, f₂, and ΔL. However, in individual distance measurement apparatuses, the correction amount Δx does not always coincide with a design value due to variations in optical systems, LEDs, and PSDs, or variations in their assembly positions. In the embodiment shown in Fig. 5, the resistance of the semifixed resistor 14 is changed to adjust and input the correction amount Δx. This adjustment is performed during, e.g., the steps in the manufacture of a camera. A method of setting the correction amount Δx is not limited to the semifixed resistor 14. A method using a semiconductor memory, e.g., a method of directly writing the correction amount Δx in an EPROM, may be employed. The operation of this embodiment will be described with reference to the flow chart shown in Fig. 8. When a photographer lightly depresses the release button by the first stroke, the switch S₁ is turned on (S-1), and a light emission instruction is output from the microcomputer 11 to the driver 13. Thus, the drive pulse signal is supplied from the driver 13 to the light emitting portions L₃ of the LED 12, thereby emitting infrared light pulses for far-distance measurement (S-2). The infrared light pulses are projected forward through the light projecting lens 1, are then reflected by the object 4, and are received on the PSD 5 through the light receiving lens 2. The currents I₁ and I₂ are output from the PSD 5 to the arithmetic processor 8. The arithmetic processor 8 checks if the output currents I₁ and I₂ are at a minimum level or higher necessary for calculation (S-3). If YES in step S-3, it is checked if the outputs from the PSD 5 are saturated (S-4). In these steps S-3 and S-4, it can be determined if the outputs from the PSD 5 fall within the dynamic range. If the outputs from the PSD 5 fall within the dynamic range, the arithmetic processor 8 calculates the distance x based on the above-mentioned equation (1) (S-5), and the distance x is A/D-converted to digital data by the A/D converter 9. The digital data is then fetched by the microcomputer 11 (S-6). The microcomputer 11 calculates the defocusing amount y based on equation (4) (S-7). If the outputs from the PSD 5 are insufficient or saturated (S-4), the arithmetic processor 8 outputs a re-emission signal to the microcomputer 11. In response to this, the microcomputer 11 outputs a re-emission instruction to the driver 13. The driver 13 causes the light-emitting portion L₄ to output infrared light pulses for near-distance measurement (S-8). The outputs from the PSD 5 become insufficient when the following two cases occur. First, the object 4 is far, and the PSD 5 cannot provide sufficient outputs. Second, the object 4 is too close, and a received LED image falls outside the PSD 5. In the former case, sufficient outputs cannot be obtained from the PSD 5 even if the light-emitting portion L₄ is operated. However, in the latter case, since an LED image can be formed within the range of the PSD 5 if the light-emitting portion L₄ is operated, it can be detected. Since the position of the light-emitting portion L₄ is located above the light-emitting portion L₃ in Fig. 5 (not at the PSD 5 side), an LED image P on the PSD 5 is received at a position near the center of the PSD 5. The reason why the outputs from the PSD 5 are saturated is that the object is too close, and light reflected by the object comes too strong. In this case, if the light-emitting portion L₄ having a lower light-emission intensity than that of the light-emitting position L₃ is operated, light reflected by the object 4 becomes weak, and the outputs from the PSD 5 can be subjected to calculation. The arithmetic processor 8 then checks if the outputs from the PSD 5 upon emission of the light-emitting portion L₄ are sufficient (S-9). If YES in step S-9, it is checked if the outputs from the PSD 5 are saturated (S-10). If NO in step S-10, the arithmetic processor 8 calculates the distance x based on the output currents (S-11). The calculation result is converted to digital data by the A/D converter 9, and is fetched by the microcomputer 11 (S-12). In this case, the distance x is obtained upon operation of the light-emitting portion L₄ and must be corrected, as described above. The correction value Δx set by the semifixed resistor 14 is fetched by the microcomputer 11 through the A/D converter 15 (S-13), and the calculated distance x is added to the correction amount Δx (S-14). The microcomputer 11 calculates the defocusing amount y using the corrected distance x (S-7). If the outputs from the PSD 5 are not sufficient even if the light-emitting portion L₄ is operated (S-9) or if the outputs are saturated (S-10), the object distance is set to be the farthest distance (e.g., an infinity) or the closest distance (e.g., 50 cm). Therefore, the defocusing amount y is set to be 0 or ymax. More specifically, when the outputs from the PSD 5 are not sufficient upon emission of the light-emitting portions L₃ and L₄, the object distance is determined to be an infinity, and the amount y is set to be 0 (S-15). If both the outputs from the PSD 5 are saturated, it is determined that the object distance is shorter than the closest distance, and the amount y is set to be ymax (S-16). The distance measurement operation is completed, as described above. When the release button is depressed still deeper, the switch S₂ is turned on (S-17), and the the photographing lens is moved by the lens actuator 10 by the defocusing amount y calculated previously (S-17). Then, the shutter is driven (S-19), thus completing a photographing operation. In the above embodiment, the light-emitting portions L₃ and L₄ of the LED 12 have a rectangular shape of an identical size, as shown in Fig. 6. However, the present invention is not limited to this. For example, the light-emitting portions L₃ and L₄ may have shapes as shown in Figs. 9A to 9C. In this case, the light-emitting portions preferably have a short width in the direction of the base line A, and are preferably elongated in a direction perpendicular to the base line A in order to reduce a distance measurement error. In the above embodiment, the light-emitting portion is used for far-distance measurement. However, both the light-emitting portions L₃ and L₄ can be emitted for the far-distance measurement, and thereafter, only the light-emitting portion L₄ can be emitted for rear-distance measurement. In this case, since light emitted from the light-emitting portion L₄ is additionally used as light for far-distance measurement, the position of the center of gravity of the LED image on the PSD 5 is offset. Therefore, the calculation result from the arithmetic processor 8 must be corrected. In the above embodiment, the light-emitting element has two light-emitting portions. However, the present invention is not limited to this. For example, a larger number of light-emitting portions or light-emitting elements may be employed as long as a camera space or optical system design allows. In this manner, more accurate distance measurement can be achieved. In the above embodiment, a light-emitting circuit is controlled such that light for far-distance measurement is emitted first, and then, light for near-distance measurement is emitted. However, the light-emission order may be reversed as needed. According to the present invention as described above, a plurality of light-emitting elements are provided at different positions in a direction of base line, and are selectively emitted by a drive means so as to output far-distance measurement light and near-distance measurement light. A light-emitting element which is arranged not at a light-receiving element side, and has a lower light emission intensity than that for far-distance measurement is used for near-distance measurement. Since light reflected by a near object can be appropriately caught, a near distance can be accurately measured. According to the present invention, since near-distance measurement light is output from a light-emitting element which is not at the side of the light-receiving element, a finder incident angle of light reflected by the object can be decreased, parallax of a finder distance measurement frame can be advantageously reduced.

Claims: A distance measurement apparatus for a camera, comprising: at least first and second light-emitting elements (L₃, L₄) disposed along a base line (A) perpendicular to the optical axis of a camera lens and disposed to emit light beams towards an object to be photographed; light receiving means (5) extended along said base line to receive a said light beam reflected by said object and to provide an electric signal (I₁, I₂) representative of the position along said receiving means at which said received light beam is incident; and arithmetic means (8) for calculating the distance to said object in accordance with said electric signal; characterised by: drive means (13) operable to cause said first light-emitting element (L₃) to selectively emit a first light beam and said second light-emitting element (L₄) to selectively emit a second light beam, said first light beam being of higher intensity than said second light beam and said first element being disposed closer than said second element to said light receiving means (5); control means (11) for controlling operation of said drive means (13) in accordance with the intensity of the light beam received by said light receiving means (5) to select said first element (L₃) when said received intensity is low and said second element (L₄) when said received intensity is relatively high, whereby said first element (L₃) is used for measurement of far distances and said second element (L₄) for relatively near distances; and correction means (14,15) for providing a correction signal effective to correct the distance calculated by said arithmetic means (8) in accordance with the element (L₃,L₄) currently selected by said drive means (13). Apparatus according to Claim 1 characterised in that said light receiving means (5) provides said electric signal having a magnitude representative of the intensity of the received light beam, and said arithmetic means (8) is operable to monitor said magnitude to determine whether said intensity is low or relatively high and to provide a signal representative of that determination to said control means (11). Apparatus according to Claim 2 characterised in that said arithmetic means (8) is operable to monitor said magnitude and calculate whether said magnitude is within a range representative of a predetermined dynamic range of said light receiving means (5) and to provide said signal representative of that determination to said control means (11). Apparatus according to Claim 3 characterised in that said arithmetic means (8) is operable to calculate whether said magnitude is above or below said range; and in the event said magnitude is below said range when said first element (L₃) is emitting said first higher intensity light beam, said arithmetic means calculates said distance as infinity; and in the event said magnitude is above said range when said second light emitting element (L₄) is emitting said second lower intensity light beam, said arithmetic means calculates said distance as a predetermined minimum distance. Apparatus according to any one of Claims 1 to 4 characterised in that each said light-emitting element is an infrared light-emitting-diode (LED).

Inventors: TAKAHASHI YOSHIHARU, TAKAHASHI, YOSHIHARU
Applicants: KONISHIROKU PHOTO IND, KONICA CORPORATION
Application year: 1988
Main classification: G01S17
IPC codes: G01S17, G02B7