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Flux Density due to a current flowing in a long straight wire

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Presentation on theme: "Flux Density due to a current flowing in a long straight wire"— Presentation transcript:

1 Flux Density due to a current flowing in a long straight wire
© D Hoult 2008

2

3

4 The field at point p is directed

5 The field at point p is directed out of the plane of the diagram (“corkscrew rule”)

6

7 The magnitude of B at point p depends on

8 The magnitude of B at point p depends on
the current, I

9 The magnitude of B at point p depends on
the current, I the perpendicular distance of p from the wire

10 The magnitude of B at point p depends on
the current, I the perpendicular distance of p from the wire the medium surrounding the wire

11 Experiments show that B a I and if r is small compared with the length of the wire then

12 Experiments show that B a I and if r is small compared with the length of the wire then 1 B a r Therefore

13 Experiments show that B a I and if r is small compared with the length of the wire then 1 B a r Therefore I B = (a constant) r

14 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation

15 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation
2 p r

16 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation
2 p r where µ is the permeability of the medium surrounding the wire

17 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation
2 p r where µ is the permeability of the medium surrounding the wire If the medium is a vacuum (or air) the permeability is written as µo

18 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation
2 p r where µ is the permeability of the medium surrounding the wire If the medium is a vacuum (or air) the permeability is written as µo The units of µ are

19 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation
2 p r where µ is the permeability of the medium surrounding the wire If the medium is a vacuum (or air) the permeability is written as µo The units of µ are T m A-1 =

20 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation
2 p r where µ is the permeability of the medium surrounding the wire If the medium is a vacuum (or air) the permeability is written as µo The units of µ are T m A-1 = NA-2

21 Because this is a situation having cylindrical symmetry, the factor 2p is included in the equation
2 p r where µ is the permeability of the medium surrounding the wire If the medium is a vacuum (or air) the permeability is written as µo The units of µ are T m A-1 = NA-2 1 N A-2 = 1 Henry per meter (H m-1)


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