• 한국산학기술학회논문지
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• 제19권12호
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• pp.910-917
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• 2018

본 논문은 무인차량 원격 제어 시 실재감과 안전성을 향상시키기 위한 기술 개발 내용을 설명한 것이다. 일반적으로 무인차량 원격 운용 장치의 경우 조이스틱 형태의 장치나 간이 조향 휠로 구성하는 것이 대부분이다. 또한 차량 또는 장비를 직접 운전하는 감성을 구현하거나 현재 주행 상황을 운용 장치로 피드백하지 않기 때문에 사용자 입장에서는 이질감을 느낄수밖에 없었다. 최근 무인화 연구가 활발해짐에 따라, 이질감과 함께 현재의 주행 상황을 운전자에게 피드백하지 않아 발생하는 위험까지 제기되었고, 이러한 문제점을 제거하기 위한 힘반향 햅틱제어 기술의 필요성이 대두되었다. 따라서 본 연구에서는 기존의 무인차량 운용 장치가 가지고 있는 문제점을 해결하기 위하여 차량의 주행 상태를 고려한 힘반향 햅틱제어 기술을 제시하였다. 고려되어진 차량 주행 상태는 첫째로 차체 옆미끄럼각(${\beta}$)과 요레이트(${\gamma}$)와 같이 상태변수와 차량 동적 거동을 나타내는 파라미터를 포함하며, 위험 구역 접근, 장애물에 의한 조향 제한 등을 나타낼 수 있는 파라미터를 포함한다. 또한 햅틱제어 기술은 크게 일반 주행 상황, 위험 구역 접근 상황, 장애물에 의한 조향 제한 상황, 제어권 전환 상황 별 알고리즘으로 구성되며, 각 상황 별 천이 과정이 자연스럽도록 알고리즘을 구성하였다. 이러한 알고리즘을 검증하기 위하여 차량동역학 해석 시뮬레이션 툴을 활용, CAN 통신으로 구성된 시뮬레이터 환경을 구축하였으며, 각 상황 별 알고리즘 동작을 평가해봄으로써 실현 가능성 및 성능을 입증하였다.

• Journal of Biosystems Engineering
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• 제3권1호
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• pp.1-19
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• 1978

Power tiller is a major unit of agricultural machinery being used on farms in Korea. About 180.000 units are introduced by 1977 and the demand for power tiller is continuously increasing as the farm mechanization progress. Major farming operations done by power tiller are the tillage, pumping, spraying, threshing, and hauling by exchanging the corresponding implements. In addition to their use on a relatively mild slope ground at present, it is also expected that many of power tillers could be operated on much inclined land to be developed by upland enlargement programmed. Therefore, research should be undertaken to solve many problems related to an effective untilization of power tillers on slope ground. The major objective of this study was to find out the travelling and tractive characteristics of power tillers being operated on general slope ground.In order to find out the critical travelling velocity and stability limit of slope ground for the side sliding and the dynamic side overturn of the tiller and tiller-trailer system, the mathematical model was developed based on a simplified physical model. The results analyzed through the model may be summarized as follows; (1) In case of no collision with an obstacle on ground, the equation of the dynamic side overturn developed was: $$\sum_n^{i=1}W_ia_s(cos\alpha cos\phi-{\frac {C_1V^2sin\phi}{gRcos\beta})-I_{AB}\frac {v^2}{Rr}}=0$$ In case of collision with an obstacle on ground, the equation was: $$\sum_n^{i=1}W_ia_s\{cos\alpha(1-sin\phi_1)-{\frac {C_1V^2sin\phi}{gRcos\beta}\}-\frac {1}{2}I_{TP} \( {\frac {2kV_2} {d_1+d_2}\)-I_{AB}{\frac{V^2}{Rr}} \( \frac {\pi}{2}-\frac {\pi}{180}\phi_2 \} = 0 $$ (2) As the angle of steering direction was increased, the critical travelling veloc\ulcornerities of side sliding and dynamic side overturn were decreased. (3) The critical travelling velocity was influenced by both the side slope angle .and the direct angle. In case of no collision with an obstacle, the critical velocity $V_c$ was 2.76-4.83m/sec at $\alpha=0^\circ$, $\beta=20^\circ$ ; and in case of collision with an obstacle, the critical velocity $V_{cc}$ was 1.39-1.5m/sec at $\alpha=0^\circ$, $\beta=20^\circ$ (4) In case of no collision with an obstacle, the dynamic side overturn was stimu\ulcornerlated by the carrying load but in case of collision with an obstacle, the danger of the dynamic side overturn was decreased by the carrying load. (5) When the system travels downward with the first set of high speed the limit {)f slope angle of side sliding was $\beta=5^\circ-10^\circ$ and when travels upward with the first set of high speed, the limit of angle of side sliding was $\beta=10^\circ-17.4^\circ$ (6) In case of running downward with the first set of high speed and collision with an obstacle, the limit of slope angle of the dynamic side overturn was = $12^\circ-17^\circ$ and in case of running upward with the first set of high speed and collision <>f upper wheels with an obstacle, the limit of slope angle of dynamic side overturn collision of upper wheels against an obstacle was $\beta=22^\circ-33^\circ$ at $\alpha=0^\circ -17.4^\circ$, respectively. (7) In case of running up and downward with the first set of high speed and no collision with an obstacle, the limit of slope angle of dynamic side overturn was $\beta=30^\circ-35^\circ$ (8) When the power tiller without implement attached travels up and down on the general slope ground with first set of high speed, the limit of slope angle of dynamic side overturn was $\beta=32^\circ-39^\circ$ in case of no collision with an obstacle, and $\beta=11^\circ-22^\circ$ in case of collision with an obstacle, respectively.