Notes 2 Spring 2005

Notes 2 Spring 2005 - Notes 2 Spring 2005.doc Scalar Fields...

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Notes 2 Spring 2005.doc Scalar Fields and Vector Fields A voltage as a function of time may be written as ( ) t v . This is an example of a function of one variable. In electromagnetics this, as well as other quantities of interest, are also often functions of time and space. In the Cartesian coordinate system we might write ( ) t , z , y , x v v The fact that this quantity is now a function of three dimensional space makes this a field . The fact that this quantity is a scalar (there is no direction associated with it) as opposed to a vector, makes this a scalar field . Another good example of a scalar field is the temperature at different locations in this room. Since vector quantities are often of interest in physics and engineering (force, velocity, momentum, current density, electric and magnetic fields, etc. …) it is reasonable to want to consider vector fields , which are similar to scalar fields except each point in space not only has a magnitude, but also has a direction associated with it, i.e., ( ) t , z , y , x E E G G G Choosing the symbol E for this example is appropriate because we are thinking about the electric field which is a vector quantity with both a magnitude and direction. Staying with the Cartesian coordinate system we can decompose this vector field into its components like this, () ( ) ( )( z ˆ t , z , y , x y ˆ t , z , y , x x ˆ t , z , y , x t , z , y , x z y x E E E E ) + + = G The three components of , , , are themselves, scalar fields, and so we can say that to describe the information in a vector field we need to keep track of three scalar fields. , , and are unit vectors (of length one) and balance the vector nature of the left hand side of the equation with the right hand side. E G x E y E z E x ˆ y ˆ z ˆ Taking derivatives of fields: The del operator, the gradient, the divergence and the curl. We can take the derivative with respect to time of either a scalar or vector field: () [] ( ) t t , z , y , x t , z , y , x dt d = v v () () ( ) ( ) z ˆ t t , z , y , x y ˆ t t , z , y , x x ˆ t t , z , y , x t , z , y , x dt d z y x + + = E E E E G 1
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Notes 2 Spring 2005.doc We can also take the derivative with respect to any of the three Cartesian * directions in space: () [] ( ) x t , z , y , x t , z , y , x dx d = v v () [] () ( ) ( ) z ˆ z t , z , y , x y ˆ z t , z , y , x x ˆ z t , z , y , x t , z , y , x dz d z y x + + = E E E E G see example 1 below Remember that a derivative gives us information about how a function is changing with respect to some variable (often a direction or time). For a scalar field , as shown above, we can take the derivative with respect to one direction, or we can create an expression (and call it the gradient of the scalar field) that shows how the scalar field is changing in each of the three directions by adding together the derivatives in each direction along and attaching the corresponding unit
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This note was uploaded on 01/20/2012 for the course EE 4460 taught by Professor Czarnecki during the Fall '10 term at LSU.

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Notes 2 Spring 2005 - Notes 2 Spring 2005.doc Scalar Fields...

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