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            <Attribute name="description">Work is the amount of energy transferred into or out of a system by a force exerted on that system over a distance. Work is a scalar quantity that may be positive, negative, or zero. Only the component of the force exerted on a system that is parallel to the displacement of the point of application of the force will change the system’s total energy. The work-energy theorem states that the change in an object’s kinetic energy is equal to the sum of the work (net work) being done by all forces exerted on the object.</Attribute>
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            <video:description>Work is the amount of energy transferred into or out of a system by a force exerted on that system over a distance. Work is a scalar quantity that may be positive, negative, or zero. Only the component of the force exerted on a system that is parallel to the displacement of the point of application of the force will change the system’s total energy. The work-energy theorem states that the change in an object’s kinetic energy is equal to the sum of the work (net work) being done by all forces exerted on the object.</video:description>
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            <Attribute name="description">If a force varies with position, the work done by that force cannot generally be calculated as a simple product. Instead, an integral is required to sum the infinitesimal work contributions along the object’s path. The work done by such a force is given by a line integral, evaluated along the path from the object’s initial to final position. For one-dimensional motion, work is equal to the area under the curve of the parallel component of force versus position.</Attribute>
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            <video:description>If a force varies with position, the work done by that force cannot generally be calculated as a simple product. Instead, an integral is required to sum the infinitesimal work contributions along the object’s path. The work done by such a force is given by a line integral, evaluated along the path from the object’s initial to final position. For one-dimensional motion, work is equal to the area under the curve of the parallel component of force versus position.</video:description>
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