Name: impulse and angular momentum in rigid bodies
Uploaded: 2025-05-22T09:06:17.000Z
Duration: 1 min 15 s
Channel: JoVE

변환 운동과 회전 운동의 조합인 일반적인 평면 운동을 겪는 강체를 생각해 보십시오.
뉴턴의 두 번째 법칙은 강체에 대한 평행 이동 방정식을 제공합니다. 여기에 시간 간격 dt를 곱하고 적분의 한계에 대해 적분하면 선형 임펄스의 원리에 대한 방정식이 생성됩니다.
선형 임펄스의 원리는 물체의 운동량 변화가 물체에 가해지는 충격에 정비례한다는 것을 분명히 합니다. 이 방정식은 세 개의 직사각형 구성 요소를 사용하여 나타낼 수 있습니다.
반면에, 회전 운동에 대한 방정식은 물체의 질량 중심과 각속도에 대한 관성 모멘트의 곱의 시간 도함수로 작성할 수 있습니다.
여기서, 관성 모멘트는 일정하며, 이 방정식을 적분 형태로 변환하면 회전 임펄스의 원리가 생성됩니다.
여기서 관성 모멘트와 강체의 각속도의 곱은 각운동량과 같으며, 이는 세 개의 직사각형 구성 요소를 사용하여 설명할 수 있습니다.

충격과 모멘트의 원리

Principle of Impulse and Moment

본질적으로 병진 운동과 회전 운동이 혼합된 평면 운동을 받는 강체를 고려할 때 뉴턴의 제2법칙을 적용하면 그러한 물체의 병진 운동에 대한 공식이 제공됩니다. 이 방정식에 시간 간격 dt를 곱한 다음 적분 한계 이상으로 적분하면 선형 충격량의 원리를 구현하는 방정식이 생성됩니다.

<img alt="equation1" src="/files/ftp_upload/15550/15550_PT_equation_001.svg" style="height: 50px;">

여기서 첨자 G는 물체의 질량 중심을 나타냅니다.

선형 충격량의 원리는 물체의 운동량 변화가 물체에 가해진 충격량에 비례한다는 것을 전달하는 개념입니다. 이 특정 방정식은 세 개의 직사각형 구성 요소를 사용하여 표현될 수 있습니다.

대조적으로, 회전 운동 방정식은 물체의 질량 중심에 대한 관성 모멘트와 각속도의 곱을 시간에 따른 변화율(시간 도함수)로 표현합니다. 이러한 맥락에서 관성 모멘트는 일정하게 유지됩니다. 이 방정식을 적분 형태로 변환하면 회전 충격량의 원리가 발생합니다.

<img alt="equation2" src="/files/ftp_upload/15550/15550_PT_equation_002.svg" style="height: 50px;">

이 원리에서 관성 모멘트와 강체의 각속도의 곱은 각운동량과 동일합니다. 이 관계는 세 개의 직사각형 구성 요소를 사용하여 설명할 수 있습니다. 따라서 이 이야기는 선형 및 회전 충격의 원리를 강조하면서 평면 운동에서 강체의 복잡한 역학을 탐구합니다.

변환 운동과 회전 운동의 조합인 일반적인 평면 운동을 겪는 강체를 생각해 보십시오.
뉴턴의 두 번째 법칙은 방정식을 제공합니다 ...

Education

교육

JoVE Core

Mechanical Engineering

기계공학

Unit 1

제1단원

3-Dimensional Kinetics of a Rigid Body

강체의 3차원 운동역학

KEY TERMS AND CONCEPTS

주요 용어 및 개념

impulse and angular momentum in rigid bodies

Impulse and angular momentum help describe a rigid body moving in a plane. This motion combines translation and rotation. The topic uses Newton's second law to connect force, momentum, and motion.

For translational motion, the equation is written for the center of mass, labeled G. When this equation is multiplied by a small time interval, dt, and integrated, it gives the principle of linear impulse. This principle shows that a change in momentum is proportional to the impulse applied to the body. The result can also be written in three rectangular components.

Rotational motion is treated in a similar way. The time rate of change of the product of the moment of inertia about the center of mass and the angular velocity gives the rotational equation. Here, the moment of inertia is constant. When this form is written as an integral, it becomes the principle of rotational impulse.

In the rotational case, the product of the moment of inertia and angular velocity is the angular momentum. This relationship can also be shown with three rectangular components. Together, these ideas describe the linear and rotational impulse behavior of a rigid body in plane motion.

Impulse and Angular Momentum in Rigid Bodies

impulse-and-angular-momentum-in-rigid-bodies

moments and product of inertia

Moment and Product of Inertia Basics

Moment of inertia and product of inertia describe how mass is distributed in a rigid body. They help show how the body responds about coordinate axes and planes. For a small mass element, the moment of inertia is found by multiplying the element's mass by the square of the shortest distance to one of the three coordinate axes. That same idea is extended to the whole body by integration. Adding the contributions of all the small mass elements gives the body's moment of inertia about that axis.

inertia tensor

Principal Axes and Moments of Inertia

The inertia tensor describes how mass is spread out in a rigid body and how that body resists rotation. It is written as a 3×3 matrix, and each entry represents a moment of inertia about a particular axis. This makes the tensor a compact way to study rotational behavior in three dimensions. The diagonal entries show the moments of inertia about the principal axes. These principal axes are the directions where the object has the least resistance to rotation. A smaller moment of inertia along...

moment of inertia about an arbitrary axis

moment-of-inertia-about-an-arbitrary-axis

Calculating Moment of Inertia on Any Axis

Moment of inertia can be calculated about any chosen axis, not just a principal axis. It depends on the mass distribution of the object along that axis. This makes it useful when an object rotates in a real machine or other setup where balance and stability matter. To find the moment of inertia about an arbitrary axis, the perpendicular distance from the axis to each mass element is needed. That distance is obtained with a cross product between the unit vector that gives the axis direction and...

angular momentum about an arbitrary axis

Angular Momentum Relative to Point P

Angular momentum relative to point P is found by adding the motion of every mass element in a rigid body. The body has mass m and a center of mass at point G. It rotates in an inertial reference frame, and the angular momentum at P comes from the cross product of each position vector and its linear momentum. To build the full expression, the velocity of each mass element is written as two parts. One part is the translational velocity of the body. The other part is the relative velocity caused...

angular momentum and principle axes of inertia

angular-momentum-and-principle-axes-of-inertia

Angular Momentum in Principal Axes

Angular momentum in a rigid body can be written using rectangular coordinates. The body’s angular momentum comes from the cross-product of each mass element’s position vector with the cross-product of the body’s angular velocity and that position vector. This gives a compact way to describe how a solid structure moves in rotation. To work with the equation more easily, the XYZ axes can be chosen as a new set of rectangular axes. These axes may be inclined at any angle to the reference frame.

principle of impulse and moment

Impulse and angular momentum help describe a rigid body moving in a plane. This motion combines translation and rotation. The topic uses Newton's second law to connect force, momentum, and motion. For translational motion, the equation is written for the center of mass, labeled G. When this equation is multiplied by a small time interval, dt, and integrated, it gives the principle of linear impulse. This principle shows that a change in momentum is proportional to the impulse applied to the...

kinetic energy for a rigid body

Rigid Body Energy from Center and Rotation

Rigid body kinetic energy in planar motion can be written using the body’s center of mass and its rotation. The solid object moves in general planar motion, and its center of mass is marked at point G. To find the kinetic energy of the i-th particle, the relative velocity definition is used with the position vector rA from point A to that particle. The kinetic energy of the whole body is built from the particles. First, a scalar product is taken. Then the expression is written in integral form.

equation of motion for a rigid body

Rigid Body Motion: Force and Moment Balance

Rigid body motion is described with both translational motion and rotational motion about the center of mass, point G. The center of mass is the point where Newton's Second Law applies to translation. It gives the linear motion of the body. The same body also has rotational motion about point G. The combined moments about the center of mass equal the rate of change of angular momentum. A moment is the turning effect caused by a force, and an external force applied away from the center of mass...

euler equations of motion

Rigid Body Rotation in Euler’s Frame

Euler’s equations of motion describe how a rigid body rotates when measured in a moving frame attached to the body. The body rotates with angular velocity ω in an inertial frame, and the attached frame rotates with angular velocity Ω. Together, these two frames help describe the motion of the rigid body around its center of mass. The total moment about the center of mass is found by adding two parts. One part is the rate of change of angular momentum about the center of mass in the rotating...

torque free motion

Mars Spin Under No Torque

Torque-free motion describes the movement of a rigid body when no external torques act on it. It can be seen in places with no outside forces or friction, such as outer space. Mars is one example of this kind of motion because it rotates in space without external torque. Mars is an axisymmetric object, which means it has an axis of symmetry. That symmetry defines the rotating z-axis. The rotating frame is set so that Mars&amp;#39;s center of mass is at the origin. This setup makes the moments...

key terms and concepts

Learn how linear impulse and rotational impulse describe rigid body motion in a plane, including center of mass, angular velocity, and angular momentum.

Impulse and Angular Momentum in Rigid Bodies | 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

Impulse and Angular Momentum in Rigid Bodies

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