Audio Engineering

(Barry) #1

38 Chapter 2


For a power of  12 dBm:


0.001 10 0.00006309 W.
1012




The voltage across 600 Ω is


EWR



0 00006309 600


0 195


.V.


Note that this  12-dBm power level can appear across any impedance and will always
be the same power level. Voltages will vary to maintain this power level. In constant-
voltage systems the power level varies as the impedance is changed. In constant-
current systems the voltage changes as the impedance varies (i.e.,  12 dBm across
8 Ω 0 00006309..V). 8 0 022


2.2 Measuring Electrical Power .....................................................................................


WEl cosθ (2.8)^


WZI^2 cosθ (2.9)^


W


E


Z





2
cosθ

where W is the power in watts, E is the electromotive force in rms volts, I is the current in rms
amperes,Z is the magnitude of the impedance in ohms [in audio (AC) circuits Z (impedance) is
used in place ofR (AC resistance)], and θ is the phase difference between E and I in degrees.


These equations are only valid for single frequency rms sine wave voltages and currents.


2.2.1 Most Common Technique



  1. Measure Z and θ.

  2. Measure E across the actual load Z so that


W E
Z




2
cosθ.
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