11.6
Trabajo y poder para el movimiento rotacional
El trabajo y el poder en el movimiento rotacional son completamente análogos al trabajo y al poder en el movimiento traslacional. El trabajo total rea…
Considere una rueda hidráulica en un estanque. El agua que cae de la tubería ejerce una fuerza sobre la rueda hidráulica formando un ángulo Φ con el vector de posición, luego el trabajo realizado por la fuerza para hacer girar la rueda a través de un ángulo pequeño, dθ, es FsinΦds.
Dado que el arco ds es igual a r por dθ, el trabajo realizado es el producto de FsinΦ y rdθ.
Recordemos que la magnitud del par es igual a rFsinΦ. Por lo tanto, al sustituir, la expresión del trabajo realizado es igual a τ por dθ.
En general, si un cuerpo rígido gira de θ1 a θ2, el trabajo total realizado en el cuerpo es igual a la integración del producto del par neto y el desplazamiento angular.
La potencia instantánea entregada por una fuerza es la velocidad a la que se realiza el trabajo por la fuerza para hacer girar un objeto alrededor de su eje fijo que tiene un par constante. Por lo tanto, la potencia se expresa como τ por dθ/dt. Dado que dθ/dt es la velocidad angular ω de la rueda, la potencia es igual al par por la velocidad angular.
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Q1: How is work calculated in rotational motion?
Work in rotational motion is calculated as the product of torque and angular displacement. When a rigid body rotates through a small angle dθ, the work done equals torque times dθ. For rotation from angle θ1 to θ2, total work is the integration of net torque over the angular displacement, analogous to force times displacement in translational motion.
Q2: What is the relationship between torque, angular velocity, and power?
Power in rotational motion equals torque multiplied by angular velocity. Since angular velocity is the rate of change of angular displacement (dθ/dt), instantaneous power represents the rate at which work is done by a force rotating an object about a fixed axis. This relationship mirrors the translational power formula of force times velocity.
Q3: Why does applying force at a distance from the axis matter for rotating objects?
Applying force at a distance from the central axis generates torque, which determines the power delivered to a rotating system. The farther the force is applied from the axis, the greater the torque produced for the same force magnitude. Since power depends on torque and angular velocity, the distance from the axis directly affects how efficiently work is done on rotating objects like a merry-go-round.
Q4: How does the waterwheel example demonstrate work in rotational motion?
In a waterwheel, falling water exerts a force at an angle to the position vector. The component of force perpendicular to the radius (FsinΦ) creates torque. As the wheel rotates through angle dθ, work done equals this torque component times the angular displacement, illustrating how force, distance, and angle combine to produce rotational work.
Q5: What are the SI units for work and power in rotational systems?
Work in rotational motion is measured in joules, the same unit as translational work. Power is measured in watts, equivalent to joules per second. These SI units apply universally to rotational systems because work and power in rotational motion are completely analogous to their translational counterparts.
Q6: How does the work-energy theorem apply to rotating rigid bodies?
The work-energy theorem for rotational motion states that total work done on a rigid body equals the change in its rotational kinetic energy. Since work is calculated as the integral of net torque over angular displacement, this theorem connects the torque applied to a body with its resulting angular acceleration and energy changes.
Q7: What is the key analogy between rotational and translational motion for work and power?
In rotational motion, torque and angular displacement are analogous to force and linear displacement in translational motion. Similarly, power in rotation equals torque times angular velocity, just as translational power equals force times velocity. This complete analogy means the mathematical relationships and physical principles governing work and power are identical in both systems.