Thursday, 16 October 2014

FUNDAMENTALS OF ELECTRIC SYSTEMS

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FUNDAMENTALS OF ELECTRIC SYSTEMS

THE MAGNETIC FIELD:
                
                                   A magnetic field is defined as the space around a magnet or a current carrying conductor. The magnetic field B is represented by lines of induction. Figure illustrates the lines of induction of a magnetic field B near a long current carrying conductor.
The vector of the magnetic field is related to its lines of induction in this way:
1.       The direction of B at any point is given by the tangent to the line of induction.
2.       The number of lines of induction per unit cross-sectional area (perpendicular to the lines) is proportional to the magnitude of B .Magnetic field B is large if the lines are close together, and it is small if they are far apart.
         The flux of magnetic field B is given by

The integral is taken over the surface for which flux is defined.
The magnetic field exerts a force on any charge moving through it. If q0 is a positive charge moving at a velocity v in a magnetic field B, the force F acting on the charge Figure is given by:

The magnitude of the force F is given by:

Where (sine) is the angle between v and B.

The force F will always be at a right angle to the plane formed by v and B. Thus, it will always be a sideways force. The force will disappear in these cases:
1.       If the charge stops moving
2.       If v is parallel or anti parallel to the direction of B
The force F has a maximum value if v is at a right angle to B (angle = 90).
Figure illustrates the force created on a positive and a negative electron moving in a magnetic field B pointing out of the plane of the figure. The unit of B is the tesla (T) or weber per square meter (Wb/m2). Thus,
The force acting on a current-carrying conductor placed at a right angle to a magnetic field B is given by:

F = ilB

Where l is the length of conductor placed in the magnetic field.
                          
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