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Work is equal to a constant force exerted on an object in the direction of motion, times the object s displacement

You probably have used the word work in many other ways For example, a computer might work well, learning physics can be hard work, and you might work at an after-school job To physicists, however, work has a very precise meaning Recall that Fd

49 Given:



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in W The right side of the equation involves the object s mass and its velocities after and before the force was exerted The quantity 1 mvi2 describes a property of the system 2 Kinetic energy What property of a system does 1 mvi2 describe A 2 massive, fast-moving vehicle can do damage to objects around it, and a baseball hit at high speed can rise high into the air That is, an object with this property can produce a change in itself or the world around it This property, the ability of an object to produce a change in itself or the world around it, is called energy The fast-moving vehicle and the baseball possess energy that is associated with their motion This energy resulting from motion is called kinetic energy and is represented by the symbol KE Kinetic Energy KE





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The kinetic energy of an object is equal to times the mass of the object 2 multiplied by the speed of the object squared

4-4B Constant capacitive reactance lines (Courtesy of Kay Elementrics)

Figure 10-2 If a planet is in a circular orbit, then the force is perpendicular to the direction of motion Consequently, the gravitational force does no work on the planet

14 15 16 17 FileWriter fw1 = new FileWriter(new File("f1txt")); FileWriter fw2 = new FileWriter(new BufferedWriter(new PrintWriter("f2txt"))); PrintWriter pw1 = new PrintWriter(new BufferedWriter(new FileWriter("f3txt"))); PrintWriter pw2 = new PrintWriter(new FileWriter(new File("f4txt")));

Substituting KE into the equation W 1 mvf2 1 mvi2 results in W KEf 2 2 KEi The right side is the difference, or change, in kinetic energy The work-energy theorem states that when work is done on an object, the result is a change in kinetic energy The work-energy theorem can be represented by the following equation

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The relationship between work done and the change in energy that results was established by nineteenth-century physicist James Prescott Joule To honor his work, a unit of energy is called a joule (J) For example, if a 2-kg object moves at 1 m/s, it has a kinetic energy of 1 kg m2/s2, or 1 J Recall that a system is the object of interest and the external world is everything else For example, one system might be a box in a warehouse and the external world might consist of yourself, Earth s mass, and anything else external to the box Through the process of doing work, energy can move between the external world and the system Notice that the direction of energy transfer can go both ways If the external world does work on a system, then W is positive and the energy of the system increases If, however, a system does work on the external world, then W is negative and the energy of the system decreases In summary, work is the transfer of energy by mechanical means

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