Chapter 4 DYNAMICS: FORCE AND NEWTON S LAWS OF MOTION Part (a) shows an overhead view of two ice skaters pushing on a third. Forces are vectors and add like other vectors, so the total force on the third skater is in the direction shown. In part (b), we see a free-body diagram representing the forces acting on the third skater.
The same force exerted on systems of different masses produces different accelerations. (a) (b) (c) A basketball player pushes on a basketball to make a pass. (The effect of gravity on the ball is ignored.) The same player exerts an identical force on a stalled SUV and produces a far smaller acceleration (even if friction is negligible). The free-body diagrams are identical, permitting direct comparison of the two situations. A series of patterns for the free-body diagram will emerge as you do more problems.
Force and Mass Mass is the measure of how hard it is to change an object s velocity. Mass can also be thought of as a measure of the quantity of matter in an object. Newton s First Law of Motion If you stop pushing an object, does it stop moving? Only if there is friction! In the absence of any net external force, an object will keep moving at a constant speed in a straight line, or remain at rest. This is also known as the law of inertia. In order to change the velocity of an object magnitude or direction a net force is required. An inertial reference frame is one in which the first law is true. Accelerating reference frames are not inertial.
Newton s Second Law of Motion Two equal weights exert twice the force of one; this can be used for calibration of a spring:
Now that we have a calibrated spring, we can do more experiments. Acceleration is proportional to force:
Acceleration is inversely proportional to mass:
Free-body diagrams: A free-body diagram shows every force acting on an object. Sketch the forces Isolate the object of interest Choose a convenient coordinate system Resolve the forces into components Apply Newton s second law to each coordinate direction
Newton s Third Law of Motion
Some action-reaction pairs:
Although the forces are the same, the accelerations will not be unless the objects have the same mass. Contact forces: The force exerted by one box on the other is different depending on which one you push.
The Vector Nature of Forces: Forces in Two Dimensions The easiest way to handle forces in two dimensions is to treat each dimension separately, as we did for kinematics.
The weight of an object on the Earth s surface is the gravitational force exerted on it by the Earth. Apparent weight: Your perception of your weight is based on the contact forces between your body and your surroundings. If your surroundings are accelerating, your apparent weight may be more or less than your actual weight.
Normal Forces The normal force may be equal to, greater than, or less than the weight.
The normal force is always perpendicular to the surface.
Summary Force: a push or pull Mass: measures the difficulty in accelerating an object Newton s first law: if the net force on an object is zero, its velocity is constant Inertial frame of reference: one in which the first law holds Newton s second law: Free-body diagram: a sketch showing all the forces on an object Newton s third law: If object 1 exerts a force on object 2, then object 2 exerts a force on object 1. Contact forces: an action-reaction pair of forces produced by two objects in physical contact Forces are vectors Newton s laws can be applied to each component of the forces independently Weight: gravitational force exerted by the Earth on an object On the surface of the Earth, W = mg Apparent weight: force felt from contact with a floor or scale Normal force: force exerted perpendicular to a surface by that surface Normal force may be equal to, lesser than, or greater than the object s weight
Normal Forces The normal force is the force exerted by a surface on an object.
The net force on a lawn mower is 51 N to the right. At what rate does the lawn mower accelerate to the right?
A sled experiences a rocket thrust that accelerates it to the right. Each rocket creates an identical thrust T. As in other situations where there is only horizontal acceleration, the vertical forces cancel. The ground exerts an upward force N on the system that is equal in magnitude and opposite in direction to its weight, w. The system here is the sled, its rockets, and rider, so none of the forces between these objects are considered. The arrow representing friction ( f ) is drawn larger than scale.
(a) The person holding the bag of dog food must supply an upward force F hand equal in magnitude and opposite in direction to the weight of the food w. (b) The card table sags when the dog food is placed on it, much like a stiff trampoline. Elastic restoring forces in the table grow as it sags until they supply a force N equal in magnitude and opposite in direction to the weight of the load.
Since motion and friction are parallel to the slope, it is most convenient to project all forces onto a coordinate system where one axis is parallel to the slope and the other is perpendicular (axes shown to left of skier). N is perpendicular to the slope and f is parallel to the slope, but w has components along both axes, namely w and w. N is equal in magnitude to w, so that there is no motion perpendicular to the slope, but f is less than w, so that there is a downslope acceleration (along the parallel axis).
An object rests on an incline that makes an angle θ with the horizontal.
When a perfectly flexible connector (one requiring no force to bend it) such as this rope transmits a force T, that force must be parallel to the length of the rope, as shown. The pull such a flexible connector exerts is a tension. Note that the rope pulls with equal force but in opposite directions on the hand and the supported mass (neglecting the weight of the rope). This is an example of Newton s third law. The rope is the medium that carries the equal and opposite forces between the two objects. The tension anywhere in the rope between the hand and the mass is equal. Once you have determined the tension in one location, you have determined the tension at all locations along the rope.
The weight of a tightrope walker causes a wire to sag by 5.0 degrees. The system of interest here is the point in the wire at which the tightrope walker is standing.
(a) (b) A view from above of two tugboats pushing on a barge. The free-body diagram for the ship contains only forces acting in the plane of the water. It omits the two vertical forces the weight of the barge and the buoyant force of the water supporting it cancel and are not shown. Since the applied forces are perpendicular, the x- and y-axes are in the same direction as F x and F y. The problem quickly becomes a one-dimensional problem along the direction of F app, since friction is in the direction opposite to F app.
(a) A traffic light is suspended from two wires. (b) Some of the forces involved. (c) Only forces acting on the system are shown here. The free-body diagram for the traffic light is also shown. (d) The forces projected onto vertical (y) and horizontal (x) axes. The horizontal components of the tensions must cancel, and the sum of the vertical components of the tensions must equal the weight of the traffic light. (e) The free-body diagram shows the vertical and horizontal forces acting on the traffic light.
(a) (b) The various forces acting when a person stands on a bathroom scale in an elevator. The arrows are approximately correct for when the elevator is accelerating upward broken arrows represent forces too large to be drawn to scale. T is the tension in the supporting cable, w is the weight of the person, w s is the weight of the scale, w e is the weight of the elevator, F s is the force of the scale on the person, F p is the force of the person on the scale, F t is the force of the scale on the floor of the elevator, and N is the force of the floor upward on the scale. The free-body diagram shows only the external forces acting on the designated system of interest the person.
A leg is suspended by a traction system in which wires are used to transmit forces. Frictionless pulleys change the direction of the force T without changing its magnitude.
The force T 2 needed to hold steady the person being rescued from the fire is less than her weight and less than the force T 1 in the other rope, since the more vertical rope supports a greater part of her weight (a vertical force).