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Principles of naval engineering - Historic Naval Ships Association

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Chapter 20. -SHIPBOARD ELECTRICAL SYSTEMSLOAOQSHUNTSERIESCOMPOUND(A)SEPARATE EXCITATION(B)SELF EXCITATIONFigure 20-15.— Types <strong>of</strong> d-c generators.147.122The operation <strong>of</strong> a d-c motor depends on theprinciple that a current-carrying conductorplaced in, and at right angles to, a magneticfield tends to move at right angles to the direction<strong>of</strong> the field. A convenient method <strong>of</strong> determiningthe direction <strong>of</strong> motion <strong>of</strong> a currentcarryingconductor in a magnetic field is byuse <strong>of</strong> the right-hand motor rule for electronflow (fig. 20-16). Extend the thumb, index finger,and second finger <strong>of</strong> the right hand at rightangles to each other, with the index fingerpointed in the direction <strong>of</strong> the flux (toward thesouth pole) and the second finger pointed in thedirection <strong>of</strong> electron flow. The thumb then pointsin the direction <strong>of</strong> motion <strong>of</strong> the conductor withrespect to the field.ALTERNATING-CURRENT THEORYJust as a current flowing in a conductorproduces a magnetic field around the conductor,the reverse <strong>of</strong> this process is true. A voltagecan be generated in a circuit by moving a conductorso that it cuts across lines <strong>of</strong> magneticforce or, conversely, by moving the lines <strong>of</strong>force so that they cut across the conductor. Ana-c generator utilizes this principle <strong>of</strong> electromagneticinduction to convert mechanical energyinto electrical energy.In the case <strong>of</strong> alternating current, electronsmove first in one direction andtheninthe other.Thus the direction <strong>of</strong> the current reversesperiodically and the magnitude <strong>of</strong> the voltage isconstantly changing. This variation in current isrepresented graphically in sine waveform infigure 20-17.The vertical projection (dotted line in fig.20-17) <strong>of</strong> a rotating vector may be used torepresent the voltage at any instant. Vector Ej^^represents the maximum voltage induced in aconductor rotating at uniform speed in a 2-polefield (points 3 and 9). The vector is rotatedcounterclockwise through one complete revolution(360°). The point <strong>of</strong> the vector describes acircle. A line drawn from the point <strong>of</strong> the vectorperpendicular to the horizontal diameter <strong>of</strong> thecircle is the vertical projection <strong>of</strong> the vector.The circle also describes the path <strong>of</strong> theconductor rotating in the bi-polar field. Thevertical projection <strong>of</strong> the vector represents thevoltage generated in the conductor at any instantcorresponding to the position <strong>of</strong> the rotatingvector as indicated by angled. Angle ^representsselected instants at which the generatedvoltage is plotted. The sine curve plotted at the12.143Figure 20-16.—Right-hand motor ruleforelectron flow.503

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