13.3
BC 멤버를 통해 핀 지지대에 연결된 의자에 앉아 있는 질량 70kg의 남자를 생각해 보세요. 남성이 직립 자세를 유지하는 경우, 구성원이 수평과 45° 각도를 만들 때 의자가 남성에 대한 수평 및 수직 반응을 결정하는 것이 과제입니다. 이 순간 남자의 속도는 5m/s…
70kg의 몸무게를 가진 남자가 의자에 앉아 있다고 생각해 보십시오. 의자는 길이가 10m인 부재 BC를 통해 핀 지지대에 연결됩니다.
남자가 항상 똑바로 앉아 있는 경우, 부재가 수평과 45°의 각도를 만들 때 의자가 남자에게 미치는 수평 및 수직 반응을 결정합니다. 이 순간 남자는 5m/s의 속도를 가지며 1m/s2로 증가합니다.
여기서 남자는 곡선 경로를 이동하고 남자의 접선 가속도는 1m/s2입니다. 사람의 수직 가속도는 접선 속도와 곡률 반경을 사용하여 계산할 수 있습니다.
다음으로, 남자의 자유물체 다이어그램을 그리고 접선 및 수직 구성 요소에 대한 운동 방정식을 작성합니다.
알려진 값을 대체하고 중력으로 인한 가속도를 10m/s2로 가정하면 필요한 반력을 가진 두 개의 방정식이 설정됩니다.
그것들을 동시에 해결하면 수평 및 수직 방향을 따라 반력의 크기가 제공됩니다.
View the full transcript and gain access to JoVE Core videos
Q1: How do you calculate normal acceleration for an object moving along a curvilinear path?
Normal acceleration is calculated using the tangential speed and the radius of curvature. The formula relates the square of the velocity to the radius of the curved path. In the chair problem, with a speed of 5 m/s and a member length of 10 m acting as the radius, normal acceleration can be determined. This component is perpendicular to the direction of motion and points toward the center of the curved path.
Q2: What is the difference between tangential and normal acceleration in curvilinear motion?
Tangential acceleration changes the speed of an object along its path, while normal acceleration changes the direction of motion. In the problem, tangential acceleration is 1 m/s², indicating the speed increases at this rate. Normal acceleration acts perpendicular to velocity, directed toward the center of curvature. Both components are essential for analyzing motion on curved paths and must be considered separately in equations of motion.
Q3: Why is a free-body diagram necessary when solving curvilinear motion problems?
A free-body diagram isolates the object and shows all forces acting on it, enabling systematic analysis of motion. For the seated man, the diagram displays weight, normal force, and reaction forces from the chair. This visual representation clarifies force directions and magnitudes, making it easier to write accurate equations of motion for tangential and normal components. Without it, force relationships become unclear and errors in problem-solving increase.
Q4: How do you set up equations of motion for normal and tangential components?
Equations of motion are derived by applying Newton's second law separately to tangential and normal directions. For the tangential direction, sum forces parallel to velocity and set equal to mass times tangential acceleration. For the normal direction, sum forces perpendicular to velocity and set equal to mass times normal acceleration. Substituting known values like mass (70 kg), accelerations, and gravity (10 m/s²) yields two equations with unknown reaction forces that can be solved simultaneously.
Q5: What role does the member angle play in determining reaction forces on the chair?
The member angle of 45° determines the orientation of the support structure and affects how forces distribute between horizontal and vertical directions. At this angle, the geometry influences both the normal and tangential components of acceleration relative to the chair's support. The angle directly impacts the direction of reaction forces the chair exerts on the man, requiring careful geometric analysis when decomposing forces into horizontal and vertical components for solving the problem.
Q6: How does increasing speed affect the normal acceleration in this curvilinear motion problem?
Normal acceleration depends on the square of the tangential speed and the radius of curvature. As speed increases from 5 m/s at a rate of 1 m/s², the normal acceleration increases proportionally to the square of the new speed. With a fixed radius of 10 m, higher speeds produce greater normal acceleration, requiring larger normal forces from the chair to maintain the curved path. This relationship demonstrates why faster motion on curves demands greater support forces.
Q7: What assumptions are made when solving for reaction forces in this chair problem?
Key assumptions include the man remaining upright throughout motion, the member BC maintaining constant length of 10 m, and gravity acting at 10 m/s². The man is treated as a point mass, and the chair provides only normal and tangential reaction forces. The curvilinear path is assumed to have a constant radius equal to the member length. These simplifications allow the problem to be solved using standard equations of motion without accounting for body rotation or deformation.