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Robert Richards Page 1 03/30/03
EMC Related Formulae
Log↔↔Linear Voltage
dBµV to Volts ( )( )20/12010 −= VdBV µ
Volts to dBµV ( ) 120log20 += VVdBµ
dBV to Volts ( )20/10 dBVV =
Volts to dBV ( )VdBV log20=
dBV to dBµV 120+= dBVVdBµ
dBµV to dBV 120−= VdBdBV µ
Log↔↔Linear Power
dBm to Watts ( )( )10/3010 −= dBmW
Watts to dBm 30)log(10 += WdBm
dBW to Watts ( )10/10 dBWW =
Watts to dBW )log(10 WdBw =
dBW to dBm 30+= dBWdBm
dBm to dBW 30−= dBmdBW
Log↔↔Linear Current
dBuA to uA
( )20/10 AdBA µµ =
uA to dBuA )log(20 AAdB µµ =
dBA to A ( )20/10 dBAA =
A to dBA )log(20 AdBA =
dBuA to dBA 120−= AdBdBA µ
dBA to dBuA 120+= dBAAdBµ
Log↔↔Linear Impedance
dB(ohms) to ohms
( )20/)(10 ohmsdBZ =
ohms to dB(ohms) ( )ZohmsdB log20)( =
Term Conversion
dBm to dBuV dBmZvdB ++= )log(1090µ
dBuV to dBm )log(1090 ZVdBdBm −−= µ
dBuA to dBm 90)log(10 −+= ZAdBdBm µ
dBm to dBuA 90)log(10 +−= ZdBmAdBµ
dBuA to dBuV )log(20 ZAdBVdB += µµ
dBuV to dBuA )log(20 ZVdBAdB −= µµ
Volts to Amps & Watts
Z
V
A =
Z
V
W
2
=
Amps to Volts & Watts ZAV *= ZAW *2
=
Watts to Volts & Amps ZWV *=
Z
W
A =
RF related, Field Strength & Power Density
dBuV/m to V/m )20/)120)/(((10/ −= mVdBmV µ
V/m to dBuV/m ( ) 120/log20/ += mVmVdBµ
dBuv/m to dBmW/m2 8.115/2/ −= mVdBmdBm µ
dBmW/m2 to dBuV/m 8.1152// += mdBmmVdBµ
dBuV/m to dBuA/m 5.51// −= mVdBmAdB µµ
dBuA/m to dBuV/m 5.51// += mAdBmVdB µµ
dBuA/m to dBpT 2/ += mAdBdBpT µ
dBpT to dBuA/m 2/ −= dBpTmAdBµ
W/m2 to V/m 377*)2/(/ mWmV =
V/m to W/m2
377
2)/(2/
mV
mW =
wound coil Flux Density
),(20
))((4
mradius
ampsturns
T
π
µ =
uT to A/m
25.1
/
T
mA
µ
=
A/m to uT )/(*25.1 mAT =µ
Robert Richards Page 2 03/30/03
Antenna (Far Field)
Gain, dBi to numeric
)10/(10 dBi
numericGain =
Gain, numeric to dBi
)log(10 numericGaindBi =
Gain, dBi to Antenna Factor
79.29)log(20 −−= dBiMHzAF
Antenna Factor to gain in dBi
79.29)log(20 −−= AFMHzdBi
Field Strength given Watts, Numeric Gain, Distance in
meters
Meters
Gainwatts
mV
numeric**30
/ =
Field Strength given Watts, dBi gain, Distance in meters
Meters
watts
mV
dBi )10/(
10**30
/ =
Transmit Power needed, given desired V/m, Antenna
numeric gain, Distance in meters.
numericGain
metersmV
watts
*30
)*/( 2
=
Transmit Power needed, given V/m, Antenna dBi gain,
Distance in meters
)10/(
2
10*30
)*/(
dBi
metersmV
watts =
Amplitude Modulation
Peak power, given CW power and modulation %.(sine wave
AM)
2
))01.0*%(1( ModWW CWpeak +=
Average power, given CW power level and modulation %
(sine wave AM)
2
))01.0*%(2(* 2
ModW
W cw
avg
+
=
Average power, given peak power and modulation %
2
2
))01.0*%(1(*2
))01.0*%(2(*
Mod
ModW
W
peak
avg
+
+
=
Current Probe
dB(ohm) to Zt (transfer impedance)
)20/)((10 ohmdB
tZ =
Zt to dB(ohm)
)log(20)( tZohmdB =
Conductance (Gt) in dB(s) to transfer impedance, (Zt) in
dB(ohms)
tGtZ −=
Transfer Impedance in Zt (dB(ohms)), to Conductance in Gt
(dB(s))
tZtG −=
Power needed for BCI Probe (50Ω), given voltage level into
50Ω load (V) and Probe Insertion Loss LI .
)10/))50/2log(10((
10
VLI
watts
+
=
Watts needed for 150 Ohm EM Clamp
)10/))150/2log(10((
10
VLI
watts
+
=
Conducted current level using current measuring probe
given probe factor in dB(ohm) and probe terminal voltage in
dBuv
)(ohmdBVdBAdB −= µµ
Conducted current level, given probe factor in Zt (ohms) and
terminal voltage in dBuv
)log(20 tZVdBAdB −= µµ
dB calculations
Compute db delta (volts) 







=
2
1log20
V
V
dB
Compute dB delta (amps) 







=
2
1log20
A
A
dB
Compute dB delta (watts) 







=
2
1log10
W
W
dB
compute new voltage w/ db delta







 +∆
=
20
)log(20(
10
givenVdB
newV
compute new wattage w/ db delta







 +∆
=
10
)log(10(
10
givenWdB
newW
Robert Richards Page 3 03/30/03
VSWR/reflection coefficient/return loss
VSWR given Fwd/Rev Power
fwd
rev
fwd
rev
P
P
P
P
VSWR
−
+
=
1
1
VSWR given reflection coefficient
ρ
ρ
−
+
=
1
1
VSWR
Reflection coefficient, ρ, given Z1/Z2 ohms
21
21
ZZ
ZZ
+
−
=ρ
Reflection coefficient, ρ, given fwd/rev power
fwd
rev
P
P
=ρ
Return Loss, given fwd/rev power








=
rev
fwd
P
P
dBRL log10)(
Return Loss, given VSWR






+
−
−=
1
1
log20)(
VSWR
VSWR
dBRL
Return Loss, given reflection coefficient
)log(20)( ρ−=dBRL
Mismatch loss, given fwd/rev power








=
− revfwd
fwd
PP
P
dBML log10)(
Mismatch loss, given reflection coefficient
)1log(10)( 2
ρ−−=dBML
Misc
Linear interpolation with log of freq
LLU
LU
LX XXX
FFLog
FFLog
Value +−= )(*
)/(
)/(
where FL = lower frequency
FU = Upper frequency
XL = Value at lower frequency
XU = Value at upper frequency
FX = Frequency of desired value
TEM Cell Power Needed
Z
HeightV
Watts
2
)5.0**(
=
where V = field strength in V/m
Z = TEM cell impedance in ohms

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Formulas2

  • 1. Robert Richards Page 1 03/30/03 EMC Related Formulae Log↔↔Linear Voltage dBµV to Volts ( )( )20/12010 −= VdBV µ Volts to dBµV ( ) 120log20 += VVdBµ dBV to Volts ( )20/10 dBVV = Volts to dBV ( )VdBV log20= dBV to dBµV 120+= dBVVdBµ dBµV to dBV 120−= VdBdBV µ Log↔↔Linear Power dBm to Watts ( )( )10/3010 −= dBmW Watts to dBm 30)log(10 += WdBm dBW to Watts ( )10/10 dBWW = Watts to dBW )log(10 WdBw = dBW to dBm 30+= dBWdBm dBm to dBW 30−= dBmdBW Log↔↔Linear Current dBuA to uA ( )20/10 AdBA µµ = uA to dBuA )log(20 AAdB µµ = dBA to A ( )20/10 dBAA = A to dBA )log(20 AdBA = dBuA to dBA 120−= AdBdBA µ dBA to dBuA 120+= dBAAdBµ Log↔↔Linear Impedance dB(ohms) to ohms ( )20/)(10 ohmsdBZ = ohms to dB(ohms) ( )ZohmsdB log20)( = Term Conversion dBm to dBuV dBmZvdB ++= )log(1090µ dBuV to dBm )log(1090 ZVdBdBm −−= µ dBuA to dBm 90)log(10 −+= ZAdBdBm µ dBm to dBuA 90)log(10 +−= ZdBmAdBµ dBuA to dBuV )log(20 ZAdBVdB += µµ dBuV to dBuA )log(20 ZVdBAdB −= µµ Volts to Amps & Watts Z V A = Z V W 2 = Amps to Volts & Watts ZAV *= ZAW *2 = Watts to Volts & Amps ZWV *= Z W A = RF related, Field Strength & Power Density dBuV/m to V/m )20/)120)/(((10/ −= mVdBmV µ V/m to dBuV/m ( ) 120/log20/ += mVmVdBµ dBuv/m to dBmW/m2 8.115/2/ −= mVdBmdBm µ dBmW/m2 to dBuV/m 8.1152// += mdBmmVdBµ dBuV/m to dBuA/m 5.51// −= mVdBmAdB µµ dBuA/m to dBuV/m 5.51// += mAdBmVdB µµ dBuA/m to dBpT 2/ += mAdBdBpT µ dBpT to dBuA/m 2/ −= dBpTmAdBµ W/m2 to V/m 377*)2/(/ mWmV = V/m to W/m2 377 2)/(2/ mV mW = wound coil Flux Density ),(20 ))((4 mradius ampsturns T π µ = uT to A/m 25.1 / T mA µ = A/m to uT )/(*25.1 mAT =µ
  • 2. Robert Richards Page 2 03/30/03 Antenna (Far Field) Gain, dBi to numeric )10/(10 dBi numericGain = Gain, numeric to dBi )log(10 numericGaindBi = Gain, dBi to Antenna Factor 79.29)log(20 −−= dBiMHzAF Antenna Factor to gain in dBi 79.29)log(20 −−= AFMHzdBi Field Strength given Watts, Numeric Gain, Distance in meters Meters Gainwatts mV numeric**30 / = Field Strength given Watts, dBi gain, Distance in meters Meters watts mV dBi )10/( 10**30 / = Transmit Power needed, given desired V/m, Antenna numeric gain, Distance in meters. numericGain metersmV watts *30 )*/( 2 = Transmit Power needed, given V/m, Antenna dBi gain, Distance in meters )10/( 2 10*30 )*/( dBi metersmV watts = Amplitude Modulation Peak power, given CW power and modulation %.(sine wave AM) 2 ))01.0*%(1( ModWW CWpeak += Average power, given CW power level and modulation % (sine wave AM) 2 ))01.0*%(2(* 2 ModW W cw avg + = Average power, given peak power and modulation % 2 2 ))01.0*%(1(*2 ))01.0*%(2(* Mod ModW W peak avg + + = Current Probe dB(ohm) to Zt (transfer impedance) )20/)((10 ohmdB tZ = Zt to dB(ohm) )log(20)( tZohmdB = Conductance (Gt) in dB(s) to transfer impedance, (Zt) in dB(ohms) tGtZ −= Transfer Impedance in Zt (dB(ohms)), to Conductance in Gt (dB(s)) tZtG −= Power needed for BCI Probe (50Ω), given voltage level into 50Ω load (V) and Probe Insertion Loss LI . )10/))50/2log(10(( 10 VLI watts + = Watts needed for 150 Ohm EM Clamp )10/))150/2log(10(( 10 VLI watts + = Conducted current level using current measuring probe given probe factor in dB(ohm) and probe terminal voltage in dBuv )(ohmdBVdBAdB −= µµ Conducted current level, given probe factor in Zt (ohms) and terminal voltage in dBuv )log(20 tZVdBAdB −= µµ dB calculations Compute db delta (volts)         = 2 1log20 V V dB Compute dB delta (amps)         = 2 1log20 A A dB Compute dB delta (watts)         = 2 1log10 W W dB compute new voltage w/ db delta         +∆ = 20 )log(20( 10 givenVdB newV compute new wattage w/ db delta         +∆ = 10 )log(10( 10 givenWdB newW
  • 3. Robert Richards Page 3 03/30/03 VSWR/reflection coefficient/return loss VSWR given Fwd/Rev Power fwd rev fwd rev P P P P VSWR − + = 1 1 VSWR given reflection coefficient ρ ρ − + = 1 1 VSWR Reflection coefficient, ρ, given Z1/Z2 ohms 21 21 ZZ ZZ + − =ρ Reflection coefficient, ρ, given fwd/rev power fwd rev P P =ρ Return Loss, given fwd/rev power         = rev fwd P P dBRL log10)( Return Loss, given VSWR       + − −= 1 1 log20)( VSWR VSWR dBRL Return Loss, given reflection coefficient )log(20)( ρ−=dBRL Mismatch loss, given fwd/rev power         = − revfwd fwd PP P dBML log10)( Mismatch loss, given reflection coefficient )1log(10)( 2 ρ−−=dBML Misc Linear interpolation with log of freq LLU LU LX XXX FFLog FFLog Value +−= )(* )/( )/( where FL = lower frequency FU = Upper frequency XL = Value at lower frequency XU = Value at upper frequency FX = Frequency of desired value TEM Cell Power Needed Z HeightV Watts 2 )5.0**( = where V = field strength in V/m Z = TEM cell impedance in ohms