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1 Markets I: The Ecosystem and Exchange-Traded Marketsবাজার অনলাইনইংরেজি 2 Markets II: Rates, FX and Creditবাজার অনলাইনইংরেজি 3 Markets III: Commodities, Energy and Cryptoবাজার অনলাইনইংরেজি 4 Quantitative Methodsপদ্ধতি অনলাইনইংরেজি 5 Derivatives and Volatilityডেরিভেটিভস অনলাইনইংরেজি 6 Rates, Credit, XVA and Riskসুদহার, ঋণ ও ঝুঁকি অনলাইনইংরেজি 7 Research Craft: Predictors, Backtests, Measurement, Portfoliosগবেষণা অনলাইনইংরেজি 8 Strategies I: Equities and Futuresকৌশল অনলাইনইংরেজি 9 Strategies II: Volatility, Relative Value, Macro and the Bank Desksকৌশল অনলাইনইংরেজি 10 Microstructure and Executionএক্সিকিউশন অনলাইনইংরেজি 11 Market Making and High-Frequency Tradingমার্কেট মেকিং অনলাইনইংরেজি 12 Machine Learning for Marketsমেশিন লার্নিং অনলাইনইংরেজি 13 Low-Latency Softwareপ্রযুক্তি অনলাইনইংরেজি 14 Networks, Hardware and Trading Infrastructureপ্রযুক্তি অনলাইনইংরেজি 15 Research, Data and Risk Platformsপ্রযুক্তি অনলাইনইংরেজি 16 The Desk and the Firmপ্রতিষ্ঠান অনলাইনইংরেজি 17 The Industry: Firms, Roles and Careersক্যারিয়ার অনলাইনইংরেজি 18 Interviews I: Maths, Probability and Speedক্যারিয়ার অনলাইনইংরেজি 19 Interviews II: Markets, Trading Games and the Final Roundক্যারিয়ার অনলাইনইংরেজি 20 Interviews III: Codeক্যারিয়ার অনলাইনইংরেজি
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Física · পরিভাষা

Dipolo linear, circuito linear কী?

Definição 6.16 Física universitária — 1.º ano · অধ্যায় 6 — Circuitos em corrente contínua: leis de Kirchhoff e teoremas

Um dipolo é linear se a sua característica é uma reta (resistor, fontes ideais e reais); um circuito feito apenas de dipolos lineares é um circuito linear. As suas incógnitas obedecem a um sistema de equações lineares (as leis de Kirchhoff mais as características), cuja solução é única.

Duas fontes alimentando uma carga comum R_3. Vista dos terminais de R_3, o resto do circuito é uma fonte de Thévenin (E_ Th, R_ Th); o teorema de Millman dá o potencial do nó N em uma linha.
Duas fontes alimentando uma carga comum R3R_3. Vista dos terminais de R3R_3, o resto do circuito é uma fonte de Thévenin (EThE_{\mathrm{Th}}, RThR_{\mathrm{Th}}); o teorema de Millman dá o potencial do nó NN em uma linha.

উদাহরণ

Exemplo 6.20 (Três caminhos para a mesma resposta)

Na figura, E1=10 VE_1 = 10\,\mathrm{V}, R1=1.0 kΩR_1 = 1.0\,\mathrm{k}\Omega, E2=5.0 VE_2 = 5.0\,\mathrm{V}, R2=2.0 kΩR_2 = 2.0\,\mathrm{k}\Omega, R3=2.0 kΩR_3 = 2.0\,\mathrm{k}\Omega. Millman: VN=(10/1+5/2+0/2)/(1+0.5+0.5)=12.5/2=6.25 VV_N = (10/1 + 5/2 + 0/2)/(1 + 0.5 + 0.5) = 12.5/2 = 6.25\,\mathrm{V}. Superposição: E1E_1 sozinha vê R2∥R3=1 kΩR_2 \parallel R_3 = 1\,\mathrm{k}\Omega, logo u=10×1/2=5 Vu = 10 \times 1/2 = 5\,\mathrm{V}; E2E_2 sozinha vê R1∥R3=0.667 kΩR_1 \parallel R_3 = 0.667\,\mathrm{k}\Omega, u=5×0.667/2.667=1.25 Vu = 5 \times 0.667/2.667 = 1.25\,\mathrm{V}; total 6.25 V6.25\,\mathrm{V}. Thévenin visto de R3R_3: EThE_{\mathrm{Th}} é a tensão em circuito aberto do divisor (E1,R1,R2,E2)(E_1, R_1, R_2, E_2): E2+(E1−E2)R2/(R1+R2)=5+5×2/3=8.33 VE_2 + (E_1 - E_2)R_2/(R_1 + R_2) = 5 + 5 \times 2/3 = 8.33\,\mathrm{V}; RTh=R1∥R2=0.667 kΩR_{\mathrm{Th}} = R_1 \parallel R_2 = 0.667\,\mathrm{k}\Omega; então u=8.33×2/2.667=6.25 Vu = 8.33 \times 2/2.667 = 6.25\,\mathrm{V}.

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