Download For a long straight wire B = ( ìo I )/ ( 2 ð r) ìo = 4 ð x 10-7

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Transcript
Chapter 29 Ampere’s Law
Recall that we first used Coulomb’s Law to calculate the electric force. Then we used F = qE and
found the value of E by using Gauss’ Law. As we saw in the last chapter with F = qvB, if the magnetic
field is known then we can easily calculate the magnetic force. Ampere’s Law helps us to find the
magnetic field.
Gauss’s Law involved flux through a surface. The current passing through a circle is used in the
simple form of Ampere’s Law to find the magnetic field.
pages 2 – 6
PHY162 will discuss these concepts.
page 7 Ampere’s Law
The formula for the strength of the magnetic field due to current in a long straight wire was developed
in Chapter 28. B = (oI ) / (2 π r)
o = 4 π x 10-7
page 8 Ampere’s Law
1. Draw a convenient closed path. A convenient path for evaluating Ampere’s Law has two
characteristics: a) the magnetic field is either zero or has a constant value on segments of the path
b) the magnetic field is either parallel or perpendicular to the path.
2. Determine the net current that penetrates the area bounded by the closed path.
3. Multiply B by the length of each segment of the path where B a) is parallel to the path, b) is not
zero, c) has a constant value. If B is anti-parallel to the path insert a negative sign on that term. You
may recognize that these comments are consistent with the calculation of a vector dot product.
4. Equate this result to o times the net current that penetrates the area.
5. Solve for B.
Figures 12, 13, 14, and 15 a,b and the accompanying reading on pages 8 -10 are worth a brief
examination but we will not need this material.
page 11 Field of a Straight Wire
We will apply the steps given above to find B for a long straight wire that has a current I.
We will work Exercises 3 and 4 in class.
pages 14 and 15 Field of a Solenoid
We will work this example in class.
Right Hand Rule for Solenoids
This is a continuation of the right hand rule we used for the long straight wire.
page 17 The Toroid
PHY162 will cover this section.
Why is coaxial cable used to carry TV (and other) signals?
pages 31-18 to 31-19
Know how to find the force for two long straight parallel wires that have current.
How is the Ampere unit defined?
Copyright© 2001 - 2006 by Greg Clements Permission is granted to reproduce this document as
long as 1) this copyright notice is included, 2) no charge of any kind is made, and, 3) the use is for an
educational purpose. Editing of the document to suit your own class style and purposes is allowed.