COKEVA 11940C Hinweis zum Betrieb - Seite 10
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3‐8. Power Density and Electric Field Calculations
3‐9. The Cokeva 11940C measures magnetic field strength. Assuming a 377‐ohm field impedance, an associated
electric field strength or a wave power density can be calculated from the magnetic field measurement. Refer to the
following equations:
E─Field Strength
Power Density
EXAMPLE:
then
E
S
3‐10. Localized Field Source
3‐11. The probe can also be used as a localized magnetic field source for locating susceptibility problems on an
electronic circuit. It is a reciprocal device; that is, a voltage fed into the unit will create a magnetic field at the dual‐
loop sensor. For this application, the maximum input power is 0.5W with a characteristic worst‐case VSWR of 3:1.
Table 2 lists characteristic magnetic field strengths developed at the probe tip using 0 dBm incident power.
Frequency
(MHz)
30
100
500
850
1000
5
(
)
µ
dB
= V
+ AF + K + 51.5
SA
m
= V
+ AF + K + 51.5
SA
(
)
mW
dB
= V
+ AF + K ‐ 104.3
SA
2
cm
where
V
= voltage in dBµ V measured on analyzer
SA
AF = 11940C Antenna Factor in dB
K = loss or gain in dB between 11940C and spectrum analyzer
(Positive value if loss, negative value if gain.)
At 100 MHz, measured V
(
)
µV
dB
= 60.3 + 44 + 51.5 = 155.8 dBµV/m = 61.7 V/m
m
(
)
mW
dB
= 60.3 + 44 – 104.3 = 0 dB
2
cm
Table 2. Characteristic Magnetic Field Strength
Input Power
(incident)
Cokeva 11940C Operation Note
(
)
µA/m
µV
= 60.3 dBµV. Let K = 0 and AF = 44 dB
SA
mW
mW
= 1
2
2
cm
cm
Magnetic Field Strength
0 dBm
0 dBm
0 dBm
0 dBm
0 dBm
(
(H ), dB (µΑ/m)
101
98
94
93
98
)
µA/m
µV