An ideal source has its negative terminal on ground

PHYSICS · Multi-part · Fermi University Physics · Electronics, Instrumentation & Communication · Circuit foundations and passive networks · Sensors, detectors and experimental instrumentation

Electronics for Measurement, Ch The resistive network: two laws, one equivalent and the loading error

Problem

An ideal 12.0 V12.0\,\mathrm{V} source has its negative terminal on ground. R1=100 ΩR_1 = 100\,\Omega runs from its positive terminal to node AA, R2=100 ΩR_2 = 100\,\Omega from AA to ground, R3=150 ΩR_3 = 150\,\Omega from AA to node BB, and R4=200 ΩR_4 = 200\,\Omega from BB to ground. The output terminals are BB and ground. ((a)) Taking AA and BB as the unknown nodes, find the open-circuit voltage at BB. Then find the short-circuit current from BB to ground, and hence RthR_{\rm th}. ((b)) Find VthV_{\rm th} and RthR_{\rm th} a second way: replace everything to the left of R3R_3 by its Thevenin equivalent at AA, then carry that equivalent on through R3R_3 and R4R_4. Check RthR_{\rm th} by source suppression as well. ((c)) A 900 Ω900\,\Omega load is proposed across the output. Predict the voltage across it and its loading error, and find the smallest load resistance that keeps the error under one per cent. ((d)) With the 900 Ω900\,\Omega load in place, find the power dissipated in R1R_1, and choose the smallest rating from 0.250.25, 0.50.5, 11 and 2 W2\,\mathrm{W} that leaves a factor of two in hand.

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