Title: Star-Delta Transformation
1Star-Delta Transformation
2Examples
- Star-to-Delta
- Page 19
- Advance Electrical Eng
- by
- Morton
3Mesh Transformation
- Examples
- From
- The application of Matrix Theory to EE
- By
- Lewis Pruce
- Chapter four page 95
4Mesh Analysis
Mesh 1 25I1 60I1 60I2 - 25I3 10
0 85 I1 60 I2 - 25 I3 10 ..(1)
5Mesh Analysis
Mesh 2 60 I2 40 I2 - 60 I1 - 40 I3 20 0 -
60 I1 100 I2 - 40 I3 - 20 .(2)
6Mesh Analysis
Mesh 3 40 I3 25 I3 10 I3 25 I1 40 I2
0 -25 I1 - 40 I2 75 I3 0 . (3)
7Mesh Analysis
- So we have our three mesh equations from the
circulating currents in the three meshes. Note we
write them down in a certain order - A I1 B I2 C I3 D
- We can represent these simultaneous equations as
a matrix equation as follows ZI E
8Mesh Analysis
- ZI E
- Can be written with values
9Mesh Analysis
Where Z11 represents impedance of loop 1 and does
not share with any other loop. Z12 is an
impedance in loop 1 that is shared with loop
2. Z13 is an impedance of the loop 1 and shared
with loop 3.
10Mesh Analysis
- Similarly each row has impedances present in the
respective loop but shared with mesh of suffix
no. of the column.
11Mesh Analysis
- The numbers on the diagonal of the matrix are
positive. These are the mesh self-impedance and
are just the sum of the impedances in each mesh. - The numbers off the diagonal represent the
total impedances from one mesh with respect to
another i.e. Z12, Z13 etc. Note there are always
two i.e. the impedance from mesh one to mesh two
is the same as from mesh 2 to mesh 1. Hence for
example Z31 is the same as Z13. - The numbers from one mesh with respect to
another are always negative. - Note that the emf are positive when aiding a
circulating current i.e. on the LHS of the mesh
and negative when opposing a circulating current
i.e. on the RHS of a mesh.
12Solution using Cramers Rule
- Find the determinant of Z matrix
That could be done by expanding either one row or
one column For 1st element i.e 85 minors are
Is evaluated (100 x 75) (-40 x -40) 5900
and is called co-factor of 85
13Solution using Cramers Rule
- The procedure is repeated for each element of the
row (column) chosen - Another thing to note is that the sign of the
number in the determinant has a pattern as
follows
14Solution using Cramers Rule
- ?R () (85) (100)(75) (-40)(-40)
- (-) (-60) (-60)(75) (-25)(-40)
- () (-25) (-60)(-40) (-25)(100)
-
- Note the signs ( - ) !!
- ?R 49000
15Solution using Cramers Rule
- The next step is to replace the coefficients of
I1 with the numbers on the right hand side of the
equation, that is the column vector of applied
e.m.f's, as follows and work out its determinant
?1 -51000
? -
16Solution using Cramers Rule
- Then for I2 and I3 and workout their
determinants. i.e - ?2 -60000
- ?3 -49000 ?
?
17Solution using Cramers Rule
- Then to workout different branch currents
- I1 ?1/ ? R -1.04 A
- I2 ? 2/ ? R -1.22 A
- I3 ? 3/ ? R -1 A
18Solution by Matrix Inversion
I Z-1 E
Which involves finding the inverse matrix Z -1
There are several methods of doing this. One
method is as follows
Where CT is the adjoint of the matrix Z and Z
is the determinant of the matrix Z
19Solution by Matrix Inversion
Finally I Z-1 E
20Solution by Matrix Inversion
We can now label the currents
21Assignment exercise
- Determine Loop branch currents using both
methodsi.e. Cramers Matrix
22Hyperlinks
- en.wikipedia.org/wiki/Mesh_analysis