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Transcript
Magnetostatics
1
If charges are moving with constant velocity, a static
magnetic (or magnetostatic) field is produced. Thus,
magnetostatic fields originate from currents
Most of the equations we have derived for the electric fields
may be used to obtain corresponding equations for
magnetic fields with some modification if the equivalent
analogous quantities are substituted.
2
Magnetostatics
Biot – Savart’s Law
dH  k
In SI units,
The magnetic field intensity dH
produced at a point P by the
differential current element Idl is
proportional to the product of Idl
and the sine of the angle
between the elementand the line
joining P to the element and is
inversely proportional to the
square of the distance R between P
and the element.
Idl sin
R2
k ,
1
4
dH  k
Idl sin
4R2
3
Magnetostatics
The field produced by a
wire can be found adding
up the fields produced by a
large number of current
elements placed head to
tail along the wire (the
principle of superposition).
4
Magnetostatics
5
Magnetostatics
Magnetic Flux Density
The magnetic flux density vector is related to the magnetic
field intensity H by the following equation
B   H,
T (tesla) or Wb/m2
where  is the permeability of the medium. Except for
ferromagnetic materials ( such as cobalt, nickel, and iron),
most materials have values of  very nearly equal to that for
vacuum,
 o  4  10 7
H/m
(henry per meter)
The magnetic flux through a given surface S is given by
   B  d s,
S
Wb (weber)
6
Magnetostatics
Magnetic Force
If a magnetostatic field is present then it exerts forces on
moving charges and on currents. If a current
element Idl is located in a magnetic field B , it experiences a
force
dF  Idl  B

This force, acting on current element Idl , is in a direction
perpendicular to the current
element and also perpendicular

to B . It is largest when B and the
 wire are perpendicular.
The force acting on a charge q moving through a magnetic
field with velocity v is given by
F  q(v  B )

The force is perpendicular to the direction of charge motion,
and is also perpendicular
to B .

7