Introduction
                
              The power radiated by an antenna is equal to the radiation 
                resistance multiplied by the antenna current squared. Measurement 
                of antenna current can be done in the 137 kHz band by for instance 
                a thermocouple ammeter or other means. The unknown factor is the 
                radiation resistance. Computer programmes for antenna simulation 
                can produce a value for the radiation resistance but proper modelling 
                the antenna is not always easy. Another problem is the influence 
                of the earth. The ground constants are seldom known and even if 
                they are it is not certain that the computer program applies them 
                in the correct way. 
               
              A more reliable 
                way of determining radiated power in the 137 kHz band is by measuring 
                the field strength near the station but outside the near field 
                region. A distance of 1 km is probably sufficient to reduce the 
                influence of the near field on the measurement sufficiently and 
                2 km is definitely safe. 
               
             | 
             
                
             | 
          
           
            |  
               At such a distance we are in the far 
                field of the antenna but near enough so that the field strength 
                does not depend on the type of ground. When a strength of the 
                electric field of E mV/M is measured the radiated power follows 
                from a simple equation: 
              P=0.0111(E*d)3 in which; (1) 
              P in watt 
              E in mV/m 
              d in kilometers 
              * means multiplication 
              The equation produces the power really radiated by the 
                antenna, in other words the power "dissipated" in the 
                radiation resistance. 
              Note that this is not the same as ERP. 
                By definition ERP is the fictitious power to be fed to a half 
                wave dipole in free space that produces the measured field 
                strength. As Rik, ON7YD, has pointed out in his e-mail of June 
                25 a short vertical (and our 137 kHz antennas are always short) 
                has a theoretical gain of a factor 1.83 (2.62 dB) over a half 
                wave dipole in free space. 
             | 
             
               So if you want to know your ERP multiply 
                the power given by equation (1) by 1.83 (or add 2.62 dB). But 
                apart from a regulations point of view I see no advantage in using 
                ERP. The actual power radiated by the antenna is what counts. 
              I have a feeling that some amateurs 
                talk about their "ERP" when they mean "radiated 
                power". Maybe I'm wrong; I hope so. 
              Most 
                field strength meters do not measure the electric but the magnetic 
                component of the electromagnetic field. But this is no problem 
                because in the far field of the antenna (where we measure) there 
                is a fixed relation between the electric and the magnetic field 
                components: 
                
              E/H=120*pi ohm=377 ohm (2) in which: 
              E in V/m and H in A/m. 
              The 
                portable field strength meter to be described is a direct conversion 
                receiver with two audio output signals. One is fed to headphones 
                for tuning the meter to the signal to be measured. The other output 
                feeds a digital multimeter. 
             |