Name: two-force body equilibrium
Uploaded: 2025-05-22T09:06:02.000Z
Duration: 1 min 30 s
Channel: JoVE

ضع في اعتبارك مصباحا معلقا عموديا من الذراعين مع تثبيت نهايته العلوية.
إذا كان عضو الذراع معزولا وعملت القوتان عند نقطتين ، A و B ، مع عدم وجود حمل بينهما ، فإنه يسمى عضوا ثنائي القوة. هنا ، تكون طبيعة القوى إما مشدودة أو ضاغطة.
لكي يكون العضو المكون من قوتين في حالة توازن ، يجب أن تكون القوتان FA و FB متساويتين في الحجم ولكنهما معاكستان في الاتجاه.
للوفاء بشرط التوازن اللحظي ، يجب أن يكون لهما FA و FB نفس خط العمل.
بشكل عام ، يمكن أن يكون للعضو المكون من قوتين قوى متعددة تعمل على النقطتين A و B والتي يتم تمثيلها كقوة ناتجة عند النقطتين A و B.
إذا كان حجم واتجاه القوة على جانب واحد معروفين ، فيمكن حساب القوة على الجانب الآخر. هذا يقلل من عدد المجهولين من معادلة التوازن.
العضو ذو القوتين ليس بالضرورة مستقيما ؛ يمكن ثنيه أو منحنيه ويستخدم لتحليل هيكل الدعامات والإطارات والآلات.

<ol>
	<li>هيبلر ، آر سي (2016). الميكانيكا الهندسية - الإحصاء والديناميكيات. هوبوكين ، نيو جيرسي: قاعة بيرسون برنتيس. ص 230.</li>
	<li>بير ، إف بي ؛ جونستون ، إي آر ؛ مازوريك ، د. إف. كرومويل ، بي جيه وسيلف ، ب. (2019). ميكانيكا المتجهات للمهندسين - الإحصاء والديناميكيات. نيويورك: ماكجرو هيل. ص 195.</li>
</ol>

الجسم الخاضع لقوتين.

Two Force Member

<div style="direction:rtl">اتزان الجسم الخاضع لقوتين هو حالة خاصة تتواجد غالبًا في التطبيقات العملية. يُعرَّف الجسم ذو القوتين على أنه جسم صلب يتعرض لقوتين خارجيتين اثنتين فقط. ولكي يكون هذا الجسم في حالة اتزان، يجب أن تكون القوتان متساويتين في المقدار، وتقعان على نفس خط التأثير، ومتعاكستين في الاتجاه. <img alt="Figure 2" src="/files/ftp_upload/14273/14273_PT_Figure_1v2.svg" style="text-align: center; height: 350px;"> ضع في الاعتبار أيًا من الألواح الموضحة التي تخضع لقوتين، F1 و F2، واللتين تؤثران عند النقطتين A وB على التوالي. إذا كان اللوح في حالة اتزان، فإن مجموع عزوم F1 و F2 حول أي محور يجب أن يكون صفرًا. بجمع العزوم حول النقطة A، يمكننا إثبات أن عزم F2 يجب أن يكون صفرًا، مما يعني أن خط تأثيرها يجب أن يمر عبر النقطة A. وبالمثل، بجمع العزوم حول النقطة B، نجد أن خط تأثير F1 يجب أن يمر عبر النقطة B. وبذلك، يكون للقوتين نفس خط التأثير، وهو الخط الذي يربط بين A وB. علاوة على ذلك، يمكن إثبات أن القوتين متساويتان في المقدار ومتعاكستان في الاتجاه. يتضح ذلك من المعادلتين ΣFx = 0 و ΣFy = 0، حيث تلغي كل قوة تأثير القوة الأخرى. عندما تؤثر عدة قوى عند النقطتين A وB، يمكن استبدال القوى المؤثرة عند A بمحصلتها F1، كما يمكن استبدال القوى المؤثرة عند B بمحصلتها F2. يمكن تعريف الجسم ذو القوتين بشكل عام على أنه جسم صلب يخضع لقوى تؤثر عند نقطتين فقط. من المهم ملاحظة أنه في جميع الحالات، يجب أن تكون المحصلتان F1 و F2 على نفس خط التأثير، ومتساويتين في المقدار، ومتعاكستين في الاتجاه لضمان اتزان الجسم.</div>

يعد توازن الجسم ثنائي القوة حالة خاصة غالبا ما تتم مواجهتها في التطبيقات العملية. الجسم ذو القوتين هو جسم صلب ...

Education

JoVE Core

Mechanical Engineering

الهندسة الميكانيكية

Unit 1

الوحدة الأولى

Equilibrium of a Rigid Body

توازن الجسم الجاسئ

KEY TERMS AND CONCEPTS

المصطلحات والمفاهيم الأساسية

two-force body equilibrium

A two-force body is a rigid body acted on by only two external forces. In equilibrium, those two forces must have the same magnitude, the same line of action, and opposite directions. This balance is what keeps the body at rest.

For a plate with forces F1 and F2 applied at points A and B, equilibrium means the sum of moments about any axis is zero. If moments are summed about point A, the moment from F2 must be zero. That means the line of action of F2 must pass through point A.

The same idea works at point B. Summing the moments about point B shows that the line of action of F1 must pass through point B. So both forces lie on the line joining A and B.

The force balance also requires ΣFx = 0 and ΣFy = 0. These equations show that the two forces have the same magnitude and opposite directions, so they cancel each other out. When several forces act at A and B, each group can be replaced by a resultant force. Those resultants must still share the same line of action, the same magnitude, and opposite directions for the body to stay in equilibrium.

Two-Force Body Equilibrium

conditions of equilibrium

Rigid Body Force Balance in Equilibrium

Rigid body equilibrium depends on a balance of external forces and moments. A rigid body is in equilibrium when it has no translational motion and no rotational motion. This happens when the net force and the net couple acting on the body are both zero. Internal forces are not used when checking equilibrium. These forces act in equal and opposite pairs inside the body, so they cancel each other. Because of that, they do not affect the overall motion or change in motion of the rigid body. The...

support reactions

Types of Structural Supports

Types of structural supports control how a coplanar force system moves and reacts under load. A coplanar force system is a set of forces that all lie in the same plane. The supports create reactions at the point of contact. These reactions help keep a structure stable under external forces. Supports work by stopping translation with an equal and opposite force. They can also stop rotation by applying a couple moment in the opposite direction. In structural design, these reactions are important...

internal forces and center of gravity

Forces Inside a Body and Balance

Internal forces and the center of gravity help explain how objects stay in balance. These mechanics ideas matter for structures, machines, and vehicles that must remain stable under different loads and conditions. Internal forces are created inside a body when its particles interact. They can appear as tension, compression, or shear forces. These forces act in collinear pairs with equal magnitude and opposite direction. Between connected parts, they cancel each other and help keep the body in...

alternative sets of equilibrium equations

alternative-sets-of-equilibrium-equations

Equilibrium Conditions for a Supported Plate

Equilibrium conditions for a supported plate are used to describe when forces and moments balance. In this state, the plate has no net movement and no rotation. Engineers use these equations to study how structures behave under external loads. In many cases, the standard equilibrium equations are enough. But some systems need an alternative set of equations to match the geometry of the support points. A rectangular plate supported at points A, B, and C is one example. For this plate, the...

two force member

A two-force body is a rigid body acted on by only two external forces. In equilibrium, those two forces must have the same magnitude, the same line of action, and opposite directions. This balance is what keeps the body at rest. For a plate with forces F1 and F2 applied at points A and B, equilibrium means the sum of moments about any axis is zero. If moments are summed about point A, the moment from F2 must be zero. That means the line of action of F2 must pass through point A. The same idea...

three force member

Solving a Three-Force Member Example

A three-force member is a rigid body acted on by three forces at three points. The forces must have concurrent lines of action. If the forces are parallel, their lines of action stay parallel instead. A dumpster provides the example used here. It is connected to a pin support at point A and to a pin on a hydraulic cylinder at point B. The hydraulic cylinder acts as a two-force member in equilibrium. The dumpster weight acts through the center of gravity, and the support reaction acts at point...

equations of equilibrium in three dimensions

equations-of-equilibrium-in-three-dimensions

Checking Force Balance in 3D Structures

Checking force balance in 3D structures is a key step when a system is at rest. The vector and scalar equations of equilibrium are used to test whether a body is stable and will not collapse or fall apart. These equations give a clear way to study the forces acting on a body. The vector equations of equilibrium require the vector sum of all external forces on a body to equal zero. They also require the vector sum of the couple moments and the moments of all forces about a point to equal zero.

support reactions in three dimensions

3D Support Types for Stability and Motion

Support reactions in three dimensions keep structures stable and in equilibrium. They stop unwanted translation and rotation, so a design can handle external forces safely and work as intended. These reactions are important in many structures and systems. A ball and socket joint is one support that allows free rotation about any axis. It does not provide a moment that resists turning. At the same time, it restricts motion in space with three reaction forces along the three dimensions. A...

constraints and statical determinacy

Constraints in Structural Equilibrium

Constraints in structural engineering control how a body can move and help keep it in mechanical equilibrium. A constraint is a restriction on motion. When the right number of constraints is used, the system can stay balanced with the fewest supports needed. A system with the proper number of supports is called statically determinate. In that case, the unknown reaction forces can be found from equations of equilibrium. These systems are the easiest to analyze and design because the forces can...

key terms and concepts

Learn how a two-force body stays in equilibrium by using moment balance, force balance, and the rules for line of action, magnitude, and direction.

Two-Force Body Equilibrium | JoVE K12

JoVE Core Mechanical Engineering offers concise, easy-to-understand animated videos covering key topics such as equilibrium, forces, truss analysis, and structural mechanics. Explore their real-world applications, and witness these concepts in action through scientist-led experiments.

mechanical engineering

Two-Force Body Equilibrium

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