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TERMODINAMIKA

FISIKA. TERMODINAMIKA. POLITEKNIK UNIVERSITAS ANDALAS. HUKUM TERMODINAMIKA. Energi Dalam ∆U = C v x ∆T Kalor ∆Q = C p x ∆T. Kalor. Energi Dalam. Kapasitas Kalor pada Tekanan Tetap. Kapasitas Kalor pada Volum Tetap. Perubahan Suhu. Perubahan Suhu. HUKUM TERMODINAMIKA. Usaha

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TERMODINAMIKA

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  1. FISIKA TERMODINAMIKA POLITEKNIK UNIVERSITAS ANDALAS

  2. HUKUM TERMODINAMIKA EnergiDalam ∆U = Cv x ∆T Kalor ∆Q = Cp x ∆T Kalor EnergiDalam KapasitasKalorpadaTekananTetap KapasitasKalorpadaVolumTetap PerubahanSuhu PerubahanSuhu

  3. HUKUM TERMODINAMIKA Usaha ∆W = P x ∆V HukumTermodinamika ∆Q = ∆U + ∆W Usaha Tekanan PerubahanVolum

  4. GAS IDEAL Pada gas ideal, berlaku : P  tekanan (atm) V  volum (liter) n  mol R  konstanta (8,314) T  temperatur (Kelvin)

  5. GAS IDEAL Pada gas ideal monoatomik : Pada gas ideal diatomik :

  6. PROSES DALAM TERMODINAMIKA • ProsesIsokhorik  Volumtetap • ProsesIsobarik  Tekanantetap • ProsesIsotermik  Temperaturtetap

  7. PROSES ISOKHORIK Grafik dan persamaan pada proses isokhorik : ∆W = P . ∆V ∆V = 0 ∆W = 0 ∆Q = ∆U + ∆W ∆Q = ∆U ∆U = Cv. ∆T ∆U = Cv. (T2-T1)

  8. PROSES ISOBARIK Grafik dan persamaan pada proses isobarik : ∆W = P . ∆V ∆W = P.(V2-V1) ∆Q = Cp.(T2-T1) ∆Q = ∆U + ∆W ∆U = ∆Q – ∆W

  9. PROSES ISOTERMIK Grafik dan persamaan pada proses isotermik : ∆U = 0 ∆Q = ∆U + ∆W ∆Q = ∆W

  10. siklus Siklus  gabungan dari beberapa proses Keterangan : Proses a  b : Isobarik Proses b  c : Isokhorik Proses c  a : Isotermik

  11. CONTOH SOAL Suatu gas ideal monotomik sebanyak 1 mol mengalami proses–proses seperti pada grafik berikut : Tentukan : Pcdan Ta Wabca

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