US 7,499,829 B2
Laser rangefinder and method thereof
Seok-Hwan Lee, Incheon (Korea, Republic of); Jae-Young Lee, Seoul (Korea, Republic of); Ki-Choul Nam, Seongnam (Korea, Republic of); Kyung-Mok Kang, Incheon (Korea, Republic of); and Geun-Sik Yoo, Incheon (Korea, Republic of)
Assigned to A&D Engineering Co., Ltd, Daerim-Dong, Yeongdeungpo-gu, Seoul (Korea, Republic of)
Appl. No. 10/564,207
PCT Filed Aug. 20, 2003, PCT No. PCT/KR03/01681
§ 371(c)(1), (2), (4) Date Dec. 18, 2006,
PCT Pub. No. WO2005/006016, PCT Pub. Date Jan. 20, 2005.
Claims priority of application No. 10-2003-0046882 (KR), filed on Jul. 10, 2003.
Prior Publication US 2007/0255525 A1, Nov. 01, 2007
Int. Cl. G01B 5/02 (2006.01); G01B 5/14 (2006.01); G01B 7/02 (2006.01); G01B 7/14 (2006.01); G01B 11/02 (2006.01); G01B 11/14 (2006.01); G01B 13/02 (2006.01)
U.S. Cl. 702—159 11 Claims
OG exemplary drawing
 
1. A method for finding a range, comprising:
(a) receiving laser beams reflected from a target, and converting the same into a corresponding photocurrent signal, and converting the signal into a voltage signal;
(b) canceling a noise component from the voltage signal and converting the noise-cancelled voltage signal into range-finding data;
(c) sequentially storing the range-finding data;
(d) adding the stored range-finding data and previously processed and stored accumulated data, and storing results as accumulated data;
(e) detecting data exceeding a threshold value from among the accumulated data as target signals; and
(f) reading a target range based on the detected target signals, wherein
(a) through (d) are repeated N times, and the accumulated data in (e) are obtained by repeating (a) through (d) N times,
whrerin (b) further includes differentiating the voltage signal to cancel a voltage component that corresponds to the noise component and is superimposed on the voltage signal; and
filtering the differentiated signal with a predetermined frequency bandwidth identical to a frequency band of the target signal,
wherein the bandwidth satisfies 0.35/tr wherein tr is a rising time of a laser pulse, and a cut-off frequency satisfies ½τ wherein τ is a full width at half the maximum.