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

Considere un cuerpo rígido que experimenta un movimiento plano general, una combinación de movimiento de traslación y rotación.
La segunda ley de Newton da la ecuación del movimiento de traslación para un cuerpo rígido. Al multiplicarlo por el intervalo de tiempo dt e integrarlo sobre los límites de la integración, se obtiene una ecuación para el principio de impulso lineal.
El principio del impulso lineal articula que el cambio en el momento de un objeto es directamente proporcional al impulso ejercido sobre él. Esta ecuación se puede representar usando tres componentes rectangulares.
Por otro lado, la ecuación para el movimiento de rotación se puede escribir como la derivada del tiempo del producto del momento de inercia alrededor del centro de masa del objeto y su velocidad angular.
Aquí, el momento de inercia es constante; transformando esta ecuación en una forma integral da como resultado el principio de impulso de rotación.
Aquí, el producto del momento de inercia y la velocidad angular del cuerpo rígido es igual al momento angular, que se puede representar usando tres componentes rectangulares.

principio de impulso y momento

Principle of Impulse and Moment

Cuando se considera un cuerpo rígido que experimenta un movimiento plano, que es esencialmente una combinación de movimiento de traslación y rotación, la aplicación de la segunda ley de Newton proporciona la fórmula para el movimiento de traslación de dicho cuerpo. Si esta ecuación se multiplica por un intervalo de tiempo, dt, y luego se integra sobre los límites de integración, se obtiene una ecuación que incorpora el principio del impulso lineal.

<img alt="Equation 1" src="/files/ftp_upload/15550/15550_PT_equation_001.svg" style="text-align: center; height: 50px;">
Aquí el subíndice G representa el centro de masa del objeto.

El principio de impulso lineal es un concepto que comunica que la alteración en el impulso de un objeto es proporcional al impulso que se le aplica. Esta ecuación particular se puede representar mediante el uso de tres componentes rectangulares.

En contraste, la ecuación del movimiento de rotación se expresa como la tasa de cambio en el tiempo (derivada del tiempo) del producto del momento de inercia alrededor del centro de masa del objeto y su velocidad angular. En este contexto, el momento de inercia permanece constante. Si esta ecuación se transforma en una forma integral, resulta el principio del impulso rotacional.

<img alt="Equation 2" src="/files/ftp_upload/15550/15550_PT_equation_002.svg" style="text-align: center; height: 50px;">
En este principio, el producto del momento de inercia y la velocidad angular del cuerpo rígido equivale al momento angular. Esta relación se puede ilustrar utilizando tres componentes rectangulares. Así, esta narrativa explora la intrincada dinámica de un cuerpo rígido en movimiento plano, destacando los principios del impulso lineal y rotacional.

Principio de impulso y momento

Considere un cuerpo rígido que experimenta un movimiento plano general, una combinación de movimiento de traslación y rotación.
La segunda ley de Newton da la ecuación ...

Education

Educación

JoVE Core

Mechanical Engineering

Ingeniería Mecánica

Unit 1

Unidad 1

3-Dimensional Kinetics of a Rigid Body

Cinética tridimensional de un cuerpo rígido

KEY TERMS AND CONCEPTS

TÉRMINOS Y CONCEPTOS CLAVE

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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