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B-H ANALYZER SY-8218
/ SY-8219
8
■
2.2 Expressions to calculate measurement values
●
The following is explanation of expressions to calculate values measured by this product.
This product uses two measurement modes of Normal mode and
μ
mode
,
and Table 2-1 shows measurement values displayed in each
calculation mode.
The calculation difference point of Normal mode and
μ
mode is the following. In
μ
mode, the complex permeability from fundamental wave
element of intensity of the magnetic field H and magnetic flux density B is calculated. In Normal mode, the value which is not calculated by using
them is calculated. Refer to the following expressions for details
Table 2-1 Calculation modes and measurement values
Units in [ ] are typical. The symbol to which
*
adheres is calculated from the fundamental wave element.
Calculation
modes
Normal mode
μ
mode
Symbol
Typical
unit
Meaning
Symbol
Typical
unit
Meaning
Measureme
nt val
ues
Pcv [W/m
3
]
Core loss per volume
Bm
[T]
Max. magnetic flux
density
Pcm
[W/kg]
Core loss per mass
V
2
m
[V]
Max. induced voltage
θ
[deg]
Phase angle
Hm
[A/m]
Max. magnetic field
μ
a
-
Relative
permeability
I
1
m
[A]
Max. exciting current
Bm [T]
Max. magnetic flux
density
μ
a
-
Relative
permeability
V
2
m
[V]
Max. induced voltage
*
L
[H] Inductance
Br [T]
Residual magnetic flux
density
*
R
[
Ω
] Resistance
Hm
[A/m]
Max. magnetic field
*
|Z|
[
Ω
] Impedance
Hc [A/m]
Coercive
force
Pc
[W] Core
loss
Pc [W]
Core
loss
*
μ′
-
Complex permeability
(real part)
VA [VA]
Apparent
power
*
μ″
-
Complex permeability
(imaginary part)
I
1
m [A]
Max. exciting current
*
μ
z
-
Impedance
permeability
Br/Bm
-
Rectangular ratio
*
θ
[deg] Phase
angle
2
Φ
m [Wb]
Total flux linkage
*
Q
-
Quality
coefficient
-
-
-
*
tan
δ
-
Loss
coefficient
-
-
-
THD
[dB]
Total harmonic distortion
Expressions used by this product to calculate each value shown in Table 2-1 are as follows:
■
Hm, Hc, Bm, Br,
μ
a
, Br/Bm, 2
Φ
m
For symbols, see Figure 2-3.
(2.3)
(2.4)
(2.5)
(2.6)
Fig.2-3 Hm, Hc, Bm, Br,
μ
a
H
c
H
c
B
r
B
r
μ
a
B
m
B
m
H
m
H
m
2
m
m
m
H
H
H
2
m
m
m
B
B
B
2
c
c
c
H
H
H
2
r
r
r
B
B
B
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