13.10.2012 Views

boylistad

boylistad

boylistad

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

This result is noticeably less than the above solution. The development<br />

of Eq. (13.37) can be found in Chapter 25.<br />

Instrumentation<br />

It is important to note whether the DMM in use is a true rms meter or<br />

simply a meter where the average value is calibrated (as described in<br />

the next section) to indicate the rms level. A true rms meter will read<br />

the effective value of any waveform (such as Figs. 13.49 and 13.61)<br />

and is not limited to only sinusoidal waveforms. Since the label true<br />

rms is normally not placed on the face of the meter, it is prudent to<br />

check the manual if waveforms other than purely sinusoidal are to be<br />

encountered. For any type of rms meter, be sure to check the manual for<br />

its frequency range of application. For most it is less than 1 kHz.<br />

13.8 ac METERS AND INSTRUMENTS<br />

The d’Arsonval movement employed in dc meters can also be used to<br />

measure sinusoidal voltages and currents if the bridge rectifier of Fig.<br />

13.62 is placed between the signal to be measured and the average reading<br />

movement.<br />

The bridge rectifier, composed of four diodes (electronic switches),<br />

will convert the input signal of zero average value to one having an<br />

average value sensitive to the peak value of the input signal. The conversion<br />

process is well described in most basic electronics texts. Fundamentally,<br />

conduction is permitted through the diodes in such a manner<br />

as to convert the sinusoidal input of Fig. 13.63(a) to one having the<br />

appearance of Fig. 13.63(b). The negative portion of the input has been<br />

effectively “flipped over” by the bridge configuration. The resulting<br />

waveform of Fig. 13.63(b) is called a full-wave rectified waveform.<br />

V m<br />

–V m<br />

v i<br />

0 � 2� �<br />

0 � 2� �<br />

(a)<br />

V m<br />

v movement<br />

(b)<br />

FIG. 13.63<br />

(a) Sinusoidal input; (b) full-wave rectified signal.<br />

V dc = 0.637V m<br />

The zero average value of Fig. 13.63(a) has been replaced by a pattern<br />

having an average value determined by<br />

2Vm � 2Vm 4Vm 2Vm G ��� �����0.637Vm 2p<br />

2p p<br />

The movement of the pointer will therefore be directly related to the<br />

peak value of the signal by the factor 0.637.<br />

Forming the ratio between the rms and dc levels will result in<br />

V rms<br />

� Vdc<br />

0.707Vm �� � 1.11<br />

0.637Vm<br />

ac METERS AND INSTRUMENTS ⏐⏐⏐ 551<br />

+<br />

v i<br />

–<br />

v movement<br />

–<br />

+<br />

FIG. 13.62<br />

Full-wave bridge rectifier.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!