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It talks about fluid statics and some lectures in general physics
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Introduction This lesson is devoted to the very important concepts of work and energy. These two quantities are scalars and so have no direction associated with them, which often makes them easier to work with than vectors. In this lesson, and the next we discuss an alternative analysis of the translational motion of objects in terms of the quantities energy and momentum. The significance of energy is that they are conserved. That is, in quite general circumstances they remain constant. Learning Outcomes After successful completion of this lesson, you should be able to:
If the force and the displacement are not in the same direction, as shown in the diagram below, then the work done by the applied force is given by NOTE There will be no work done if the displacement and the applied force are at right angles with each other, since cos90^0 = 0. If the applied force does work by moving the body in the direction of the force, the work done is positive. If the body moves in the opposite direction of the force, the work is done by the body and is negative. In General, There Are Three Ways On How Work Is Done. ✓ If the force is just to impart uniform motion on the body, the force of friction has done the same amount of work. ✓ In changing the position or configuration of the body system, as in the case of force applied on a body to raise the body on an inclined plane. ✓ In imparting acceleration to the body or system. Conversion: 1 Joule = 107 Ergs 1 foot-pound = 1.356 Joules Sample Problems with Solutions:
3.2.1 Potential Energy An object may store energy because of its position. The energy that is stored is called Potential Energy (PE), because in the stored state, it has the potential to do work. 3.2.1.1 Gravitational Potential Energy Work is required to lift objects against the earth’s gravity. The potential energy due to elevated positions is called Gravitational Potential Energy. The amount of gravitational potential energy possessed by an elevated object is equal to the work done against gravity on lifting it. If a mass m is raised from position 1 to position 2, a distance h , as shown in the diagram on the right, work is done on the body against gravity with the magnitude,
Where: mg is the force and the negative sign signifies a force against gravity. If the body is allowed to fall, the weight of the body will do the same amount of work,
which in another way, is called the Potential Energy Of The Body. In other words, energy was stored in the body by virtue of its position relative to the surface. Therefore,
Since : weight w = mg , PE = wh
Consider now the work done in dragging a body of mass m along a frictionless inclined plane, as shown. Since the component of the vertical force, (the weight = mg ) along the plane is ( mg sin), the work done against this component of the weight along the plane of length L is, Note: That the height h is the distance above some reference level, such as the ground or the floor of a building. The potential energy or the work done on a body raised to a height is independent of the path, or course, taken by the body. The potential energy is relative to some reference level and depends only on mg and the height h****. The potential energy of a body at high altitude with respect to the surface of the earth is given by Where: Universal Gravitational constant , M is the mass of the earth, m is the mass of the body, R is the radius of the earth, and r is the distance of the body from the center of the earth. Note: that r is not just the altitude above the earth’s surface but includes the radius of the earth as well.
3.2.3 Transformation and Conservation of Energy Energy is given to a body or system of bodies when work is done upon it. In this process, there is merely a transfer of energy from one body to another. “ In such transfer no energy is created nor destroyed: it merely changes from one form to another. “ This statement is known as the law of conservation of energy. An example of the law of the conservation of energy is the conservation of mechanical energy (potential and kinetic) in the case of a simple pendulum of mass m. If the pendulum is raised to a height h , it acquires potential energy. When it reaches the lowest point of the arc, its potential energy is minimum, but its velocity is maximum showing that the potential energy of the pendulum has been converted to kinetic energy. This conservation is 100% ; friction at the point of support and air resistance is neglected. The Kinetic Energy at the lowest point will carry the pendulum to the same height in the other side of the swing. The law of conservation of energy still holds even if friction and air resistance are taken into account, because in that case, when the body eventually stops swinging after some time, both its potential and kinetic energies, by then, will all have been dissipated into Heat Energy. Sample Problems with Solutions:
In the MKS system, the unit of power is in joule per second , also known as the Watt , named after James Watt. In the CGS system, the unit of power is in erg per second. In the English system, the standard unit of power is the Horsepower (Hp). Sample Problems with Solutions: