application of newton’s lawsnsmn1.uh.edu/cratti/phy1301-spring2015_files/ch6_claudia.pdf ·...
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APPLICATION OF NEWTON’S LAWS Chapter 6
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• Frictional forces
• Strings and springs
• Translational Equilibrium
• Connected objects
• Circular Motion
Units of Chapter 6
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6-1 Frictional forces
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• Friction has its basis in surfaces that are not completely smooth:
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6-1 Frictional forces
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• Types of frictional forces:
• Kinetic friction: the friction experienced by surfaces sliding against one another (object is moving)
• Static friction: the friction experienced by surfaces when the object is not in motion (object is not moving)
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6-1 Frictional forces
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• Kinetic friction:
• Is a vector;
• Occurs between two objects;
• One or both objects are in motion;
• Occurs at the point of contact between surfaces;
• Opposes motion, i.e. if object is sliding to the right, kinetic friction points to the left
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6-1 Frictional forces
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• Kinetic friction:
• The kinetic frictional force depends on the normal force:
• The constant is called the coefficient of kinetic friction.
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6-1 Frictional forces
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6-1 Frictional forces
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• The kinetic frictional force is independent of the relative speed of the surfaces, and of their area of contact.
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6-1 Frictional forces
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• Static friction:
• Is a vector;
• Occurs between two objects;
• Objects are NOT in motion;
• Occurs at the point of contact between surfaces;
• Opposes direction motion would occur, i.e. if a force is applied to the right of an object but it does not move, static friction points to the left (opposite direction object would move)
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6-1 Frictional forces
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• The static frictional force has a maximum value, but may take on any value from zero to the maximum, depending on what is needed to keep the sum of forces zero.
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6-1 Frictional forces
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where
The static frictional force is also independent of the area of contact and the relative speed of the surfaces.
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6-2 Strings and springs
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• When you pull on a string or rope, it becomes taut. We say that there is tension in the string.
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6-2 Strings and springs
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• The tension in a real rope will vary along its length, due to the weight of the rope.
• Here, we will assume that all ropes, strings, wires, etc. are massless unless otherwise stated.
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6-2 Strings and springs
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• An ideal pulley is one that simply changes the direction of the tension:
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6-2 Strings and springs
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• Hooke�s law for springs states that the force increases with the amount the spring is stretched or compressed:
• The constant k is called the spring constant.
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Example Copyright © 2010 Pearson Education, Inc.
• (a) If forces of 5.0 N applied to each end of a spring cause the spring to stretch 3.5 cm from its relaxed length, how far does a force of 7.0 N cause the same spring to stretch?
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Example continued Copyright © 2010 Pearson Education, Inc.
• (b) What is the spring constant of this spring?
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6-3 Translational equilibrium
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• When an object is in translational equilibrium, the net force on it is zero:
• This allows the calculation of unknown forces.
(6-5)
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6-3 Transational equilibrium
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6-4 Connected objects
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• When forces are exerted on connected objects, their accelerations are the same.
• If there are two objects connected by a string, and we know the force and the masses, we can find the acceleration and the tension:
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6-4 Connected objects
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• We treat each box as a separate system:
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6-4 Connected objects
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• If there is a pulley, it is easiest to have the coordinate system follow the string:
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6-5 Circular motion
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• An object moving in a circle must have a force acting on it; otherwise it would move in a straight line.
• The direction of the force is towards the center of the circle.
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6-5 Circular motion
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• Some algebra gives us the magnitude of the acceleration, and therefore the force, required to keep an object of mass m moving in a circle of radius r.
• The magnitude of the force is given by:
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6-5 Circular motion
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• This force may be provided by the tension in a string, the normal force, or friction, among others.
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6-5 Circular motion
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6-5 Circular motion
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• An object may be changing its speed as it moves in a circle; in that case, there is a tangential acceleration as well:
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Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc.
• Friction is due to microscopic roughness.
• Kinetic friction:
• Static friction:
• Tension: the force transmitted through a string.
• Force exerted by an ideal spring:
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Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc.
• An object is in translational equilibrium if the net force acting on it is zero.
• Connected objects have the same acceleration.
• The force required to move an object of mass m in a circle of radius r is: