13.3
体重 70 kg の男性がメンバー BC を介してピン サポートに接続された椅子に座っているとします。 男性が直立姿勢を維持している場合、課題は、椅子が水平方向に対して 45 度の角度をなしたときの椅子の水平方向および垂直方向の反応を決定することです。 この時点で、男性の速度は 5 m/s で、1…
70kgの体重の男性が椅子に座っているとします。椅子は、長さ10mのメンバーBCを介してピンサポートに接続されています。
男性が常に直立して座っている場合は、メンバーが水平に対して45°の角度を取ったときの男性に対する椅子の水平および垂直の反応を決定します。この瞬間、男性の速度は 5 m/s で、1 m/s2 で増加しています。
ここでは、男性は曲線の経路を移動し、男性の接線方向の加速度は 1 m/s2 です。人間の通常の加速度は、接線速度と曲率半径を使用して計算できます。
次に、男性の自由体図を描き、接線成分と法線成分の運動方程式を書きます。
既知の値を代入し、重力による加速度を10 m/s2と仮定すると、必要な反力を持つ2つの方程式が確立されます。
それらを同時に解くと、水平方向と垂直方向に沿った反力の大きさが得られます。
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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.