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The Magnetic Field

When we began to study electric forces we introduced the concept of the electric field, $\vec{E}$ . In particular, we had the fundamental relation between the force on a charge q in an electric field: $\vec{F}$ = q $\vec{E}$ . We will introduce a magnetic field in a similar manner. Before doing this, however, we define what is known as the cross product $\vec{V_1}$ x $\vec{V_2}$ between two vectors $\vec{V_1}$ and $\vec{V_2}$ . Consider two such vectors in the plane of this page with an angle $\theta$ between them, as in Fig. 1.1.

**Figure 1.1:** Two vectors
$\begin{figure} \begin{center} \leavevmode \epsfxsize=2.3 in \epsfbox{/export/home/fyde/randy/figs/fig19-1.eps}\end{center}\end{figure}$

$\vec{V_1}$ x $\vec{V_2}$ , which itself is a vector, is defined as follows:

the magnitude of $\vec{V_1}$ x $\vec{V_2}$ is given by

| $\displaystyle\vec{V_1}$ x $\displaystyle\vec{V_2}$ | = | $\displaystyle\vec{V_1}$ | $\displaystyle\vec{V_2}$ | sin $\displaystyle\theta$ $\displaystyle\equiv$ V₁V₂sin $\displaystyle\theta$ , (1)
where | $\vec{V}$ | $\equiv$ V denotes the magnitude of a vector $\vec{V}$ .
$\vec{V_1}$ x $\vec{V_2}$ is a vector perpendicular to both $\vec{V_1}$ and $\vec{V_2}$ whose direction is given by the right-hand rule:
Point the thumb of your right hand in the direction of $\vec{V_1}$ and your fingers in the direction of $\vec{V_2}$ . The direction of $\vec{V_1}$ x $\vec{V_2}$ then is directed out of the palm of your hand.

As the cross product of two vectors is three dimensional in nature, it is convenient to introduce the following notation for use on our two dimensional paper. We represent a vector perpendicular to the plane of this page which is directed out of the page as a circle with a black dot in the center - this can be thought of as the tip of an arrow coming towards you. On the other hand, a vector perpendicular to the plane of this page which is directed into the page is represented as a circle with a cross through the center - this can be thought of as the tail of an arrow heading away from you. Examples of this are in Fig. 1.2.

**Figure 1.2:** Cross product of two vectors
$\begin{figure} \begin{center} \leavevmode \epsfxsize=2.7 in \epsfbox{/export/home/fyde/randy/figs/fig19-2.eps}\end{center}\end{figure}$

We note two general features of the cross product:

$\vec{V_1}$ x $\vec{V_2}$ = - $\left[\vec {V_2}\times \vec {V_1}\right]$
$\vec{V_1}$ x $\vec{V_2}$ = 0 if $\vec{V_1}$ and $\vec{V_2}$ are parallel or antiparallel, as in these cases the angle $\theta$ between the two vectors is either 0^o or 180^o, for which the magnitude of $\vec{V_1}$ x $\vec{V_2}$ given by Eq.(1.1) vanishes.

We now consider a charge q moving at velocity $\vec{v}$ . If this charge is in a magnetic field $\vec{B}$ , then it experiences a force given by

$\displaystyle\vec{F}$ = q $\displaystyle\vec{v}$ x $\displaystyle\vec{B}$ . (2)

From this we see that the units of $\vec{B}$ are N $\cdot$ s/(m $\cdot$ C), which are given the special name Tesla (T). We note that, analogous to the electric field, for a given velocity $\vec{v}$ and a given magnetic field $\vec{B}$ the force on a positive charge is in the opposite direction to the force on a negative charge.

Next: Motion of a Charged Up: Magnetism Previous: Magnetism

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10/9/1997

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