Magnetic Circuit: Difference between revisions

From Class Wiki
Jump to navigation Jump to search
No edit summary
 
(11 intermediate revisions by 2 users not shown)
Line 1: Line 1:
=Author: John Hawkins=
==Problem Statement==
==Problem Statement==


Line 8: Line 9:
First, we note that the problem statement is incomplete. Assume that the core has a relative permeability of 500. Hence, for all magnetic sections excluding the air gap,
First, we note that the problem statement is incomplete. Assume that the core has a relative permeability of 500. Hence, for all magnetic sections excluding the air gap,


<center><math>\mu=\mu_r\mu_0=(500)(4\pi\times10^{-7})</math></center>
<center><math>\mu=\mu_r\mu_0=(500)(4\pi\times10^{-7})=6.2832\times10^{-4}</math></center>


Also, as recommended in the text, we will neglect fringing.
Also, as recommended in the text, we will neglect fringing.
Line 18: Line 19:
! '''Section''' !! fg !! def !! ghc !! dc !! dabc
! '''Section''' !! fg !! def !! ghc !! dc !! dabc
|-
|-
| Length <math>l</math> (m)|| 0.01 || 0.555|| 0.555 || 0.48 || 1.4
| Length <math>l</math> (m)|| 0.01 || 0.555|| 0.555 || 0.48 || 1.38
|-
|-
| Area <math>A</math> (m<sup>2</sup>) || 0.0032 || 0.0032 || 0.0032 || 0.0096 || 8.0e-4
| Area <math>A</math> (m<sup>2</sup>) || 0.0032 || 0.0032 || 0.0032 || 0.0096 || 8.0e-4
|}
|}


We must now work backward from the air-gap, since the value of the flux-density is given there. All units are understood to be standard units.
We must now work backward from the air-gap, since the value of the flux-density is given there. We need only employ the analagous equations to Ohm's Law, KVL, and KCL. All units are standard units.
<br />

'''Air Gap:'''
'''Air Gap:'''


<br />
<math>\mathcal{R}=\frac{l_{fg}}{\mu A_fg} = 4973.6</math>


<center>
<math>\Phi_{fg}=B_{fg}A_{fg}=3.2\times10^{-4}</math>
<math>\mathcal{R}_{fg}=\frac{l_{fg}}{\mu A_{fg}} = 4973.6</math>
<br />
<math>\Phi_{fg}=B_{fg}A_{fg}=3.20\times10^{-4}</math>
<br />
<math>\mathcal{F}_{fg}=\mathcal{R}_{fg}\Phi_{fg}=1.5915</math>
</center>


<br />
<math>\mathcal{F}=\mathcal{R}_{fg}\Phi_{fg}=1.5915</math>
<br />
<br>'''Right Arms:'''
'''Right Arms:'''
<br />


<center>
<math>\Phi_{def}=\Phi_{ghc} = \Phi_{fg} = 3.2\times10^{-4}</math>
<math>\Phi_{def}=\Phi_{ghc} = \Phi_{fg} = 3.20\times10^{-4}</math>
<br />
<math>\mathcal{R}_{def}=\mathcal{R}_{ghc}=\frac{l_{def}}{\mu A_{def}}=2.7603\times10^5</math>
<br />
<math>\mathcal{F}_{def}=\mathcal{F}_{ghc}=\mathcal{R}_{def}\Phi_{def}=88.331</math>
</center>


<br />
<math>\mathcal{R}_{def}=\mathcal{R}_{ghc}=\frac{l_{def}}{\mu A_{def}}=276030</math>
<br />
'''Center Column:'''
<br />
<center>


<math>\mathcal{F}_{def}=\mathcal{F}_{ghc} = \mathcal{R}_{def}\Phi_{def}=88.331</math>
<math>\mathcal{F}_{dc}=\mathcal{F}_{def}+\mathcal{F}_{fg}+\mathcal{F}_{ghc}=178.25</math>
<br />
<math>\mathcal{R}_{dc}=\frac{l_{dc}}{\mu A_{dc}}=79,577</math>
<br />
<math>\Phi_{dc}=\frac{\mathcal{F}_{dc}}{\mathcal{R}_{dc}}=0.0022</math>
</center>


<br />
'''Center Column'''
<br />
'''Left Arm:'''
<br />
<center>


<math>\mathcal{F}_{dc}=\mathcal{F}_{def}+\mathcal{F}_{fg}+ \mathcal{F}_{ghc}=178.25</math>
<math>\ \Phi_{dabc}=\Phi_{dc}-\Phi_{def}=0.0019</math>
<br />
<math>\mathcal{R}_{dabc}=\frac{l_{dabc}}{\mu A_{dabc}}=2.745\times 10^6</math>
<br />
<math>\mathcal{F}_{dabc}=\mathcal{F}_{dabc}\Phi_{dabc}=5,271.2</math>
</center>

<br />
<br />
'''Conclusions:'''
<br />
<center>

<math>\mathcal{F}_{Total}=\mathcal{F}_{dabc}+

\mathcal{F}_{dc}+\mathcal{F}_{def}+\mathcal{F}_{fg}+

\mathcal{F}_{ghc}=5,627.7</math>
<br />
<math>\mathbf{i=\frac{\mathcal{F}_{Total}}{N}=3.52 A}</math>
</center>

<br />

Which is the quantity we were looking for.

<br />


Calculations were performed using the following [[Magnetic Circuit Matlab Script]].
Calculations were performed using the following [[Magnetic Circuit Matlab Script]].
Line 49: Line 103:


<references />
<references />

==Reviewed By==
Amy Crosby

[[Kirk Betz]]

==Read By==

==Comments==

Latest revision as of 11:42, 21 January 2010

Author: John Hawkins

Problem Statement

Img001.jpg

Problem 2.16 from Electric Machinery and Transformers, 3rd ed:

A magnetic circuit is given in Figure P2.16. What must be the current in the 1600-turn coil to set up a flux density of 0.1 T in the air-gap? All dimensions are in centimeters. Assume that magnetic flux density varies as .<ref>Guru and Huseyin, Electric Machinery and Transformers, 3rd ed. (New York: Oxford University Press, 2001), 129.</ref>

Solution

First, we note that the problem statement is incomplete. Assume that the core has a relative permeability of 500. Hence, for all magnetic sections excluding the air gap,

Also, as recommended in the text, we will neglect fringing.

The lengths and areas of each of the sections to be evaluated are given in the following table.

Table 1: Lengths and Areas for the pertinent secions of the magnetic circuit.
Section fg def ghc dc dabc
Length (m) 0.01 0.555 0.555 0.48 1.38
Area (m2) 0.0032 0.0032 0.0032 0.0096 8.0e-4

We must now work backward from the air-gap, since the value of the flux-density is given there. We need only employ the analagous equations to Ohm's Law, KVL, and KCL. All units are standard units.
Air Gap:






Right Arms:





Center Column:





Left Arm:





Conclusions:



Which is the quantity we were looking for.


Calculations were performed using the following Magnetic Circuit Matlab Script.

References

<references />

Reviewed By

Amy Crosby

Kirk Betz

Read By

Comments