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Iury Zamecki Chemin https://www.slideshare.net/IuryZameckiChemin https://www.linkedin.com/in/iury-zamecki-chemin Tabela Pares De Transformados De Laplace 𝑓(𝑡) 𝐹(𝑠) 1 Impulso Unitário 𝛿(𝑡) 1 2 Degrau Unitário 1(t) 1 𝑠 3 t 1 𝑠2 4 𝑡𝑛−1 (𝑛 − 1)! , (𝑛 = 1,2,3, … ) 1 𝑠𝑛 5 𝑡𝑛 , (𝑛 = 1,2,3, … ) 𝑛! 𝑠𝑛+1 6 𝑒−𝑎𝑡 1 𝑠 + 𝑎 7 𝑡𝑒−𝑎𝑡 1 (𝑠 + 𝑎)2 8 1 (𝑛 − 1)! 𝑡𝑛−1𝑒−𝑎𝑡 , (𝑛 = 1,2,3, … ) 1 (𝑠 + 𝑎)𝑛 9 𝑡𝑛𝑒−𝑎𝑡 , (𝑛 = 1,2,3, … ) 𝑛! (𝑠 + 𝑎)𝑛+1 10 𝑠𝑒𝑛 𝜔𝑡 𝜔 𝑠2 + 𝜔2 11 cos 𝜔𝑡 𝑠 𝑠2 + 𝜔2 12 senh 𝜔𝑡 𝜔 𝑠2 − 𝜔2 13 cosh 𝜔𝑡 𝑠 𝑠2 − 𝜔2 14 1 𝑎 (1 − 𝑒−𝑎𝑡) 1 𝑠(𝑠 + 𝑎) 15 1 𝑏 − 𝑎 (𝑒−𝑎𝑡 − 𝑒−𝑏𝑡) 1 (𝑠 + 𝑎)(𝑠 + 𝑏) 16 1 𝑏 − 𝑎 (𝑏𝑒−𝑏𝑡 − 𝑎𝑒−𝑎𝑡) 𝑠 (𝑠 + 𝑎)(𝑠 + 𝑏) Iury Zamecki Chemin https://www.slideshare.net/IuryZameckiChemin https://www.linkedin.com/in/iury-zamecki-chemin 17 1 𝑎𝑏 [1 + 1 𝑎 − 𝑏 (𝑏𝑒−𝑎𝑡 − 𝑎𝑒−𝑏𝑡)] 1 𝑠(𝑠 + 𝑎)(𝑠 + 𝑏) 18 1 𝑎2 (1 − 𝑒−𝑎𝑡 − 𝑎𝑡𝑒−𝑎𝑡) 1 𝑠(𝑠 + 𝑎)2 19 1 𝑎2 (𝑎𝑡 − 1 + 𝑒−𝑎𝑡) 1 𝑠2(𝑠 + 𝑎) 20 𝑒−𝑎𝑡𝑠𝑒𝑛 𝜔𝑡 𝜔 (𝑠 + 𝑎)2 + 𝜔2 21 𝑒−𝑎𝑡 cos 𝜔𝑡 𝑠 + 𝑎 (𝑠 + 𝑎)2 + 𝜔2 22 𝜔𝑛 √1 − 𝜁2 𝑒−𝜁𝜔𝑛𝑡𝑠𝑒𝑛 𝜔𝑛 𝑡√1 − 𝜁2 , (0 < 𝜁 < 1) 𝜔𝑛 2 𝑠2 + 2𝜁𝜔𝑛𝑠 + 𝜔𝑛2 23 − 1 √1 − 𝜁2 𝑒−𝜁𝜔𝑛𝑡𝑠𝑒𝑛 (𝜔𝑛𝑡√1 − 𝜁2 − 𝜙) 𝜙 = 𝑡𝑔−1 √1 − 𝜁2 𝜁 , (0 < 𝜁 < 1, 0 < 𝜙 < 𝜋 2 ) 𝑠 𝑠2 + 2𝜁𝜔𝑛𝑠 + 𝜔𝑛2 24 1 − 1 √1 − 𝜁2 𝑒−𝜁𝜔𝑛𝑡𝑠𝑒𝑛 (𝜔𝑛𝑡√1 − 𝜁2 + 𝜙) 𝜙 = 𝑡𝑔−1√1 − 𝜁2 𝜁 , (0 < 𝜁 < 1, 0 < 𝜙 < 𝜋 2 ) 𝜔𝑛 2 𝑠(𝑠2 + 𝑠𝜁𝜔𝑛𝑠 + 𝜔𝑛2) 25 1 − cos 𝜔𝑡 𝜔2 𝑠(𝑠2 + 𝜔2) 26 𝜔𝑡 − 𝑠𝑒𝑛 𝜔𝑡 𝜔3 𝑠2(𝑠2 + 𝜔2) 27 𝑠𝑒𝑛 𝜔𝑡 − 𝜔𝑡 cos 𝜔𝑡 2𝜔3 (𝑠2 + 𝜔2)2 28 1 2𝜔 𝑡 𝑠𝑒𝑛 𝜔𝑡 𝑠 (𝑠2 + 𝜔2)2 29 𝑡 cos 𝜔𝑡 𝑠2 − 𝜔2 (𝑠2 + 𝜔2)2 30 1 𝜔2 2 − 𝜔1 2 (cos 𝜔1 𝑡 − cos 𝜔2 𝑡) , (𝜔1 2 ≠ 𝜔2 2) 𝑠 (𝑠2 + 𝜔1 2)(𝑠2 + 𝜔2 2) 31 1 2𝜔 (𝑠𝑒𝑛 𝜔𝑡 + 𝜔𝑡 cos 𝜔𝑡) 𝑠2 (𝑠2 + 𝜔2)2
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