Created by Victoria Williams
over 6 years ago
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Question | Answer |
Heat Capacity (With and Without Mass) | ∆Q=MC∆T and ∆Q=C∆T |
1st Law of Thermodynamics (2x, one with pv) | ∆U = ∆Q - ∆W or ∆U = ∆Q - P∆V |
Ideal Gases | PV = nRT and P1V1 / T1 = P2V2 / T2 |
1st Law Thermodynamics: ISOTHERMAL | 0 = ∆Q - ∆W |
1st Law Thermodynamics: ISOCHORIC | ∆U = ∆Q - 0 |
1st Law Thermodynamics: ADIABATIC | ∆U = 0 - ∆W |
ADIABATIC EQUATION | P∆V + V∆P = nR∆T |
Kinetic Theory Equation | PV = 1/3nmV^2 |
Relationships between Cv and Cp (2x) | R = Cp - Cv and Gamma (y) = Cp/Cv |
KE of Molecules using kinetic theory (3x equations) | U = 1/2NmV^2 U = 3/2PV U = 3/2nRT |
The mean speed squared equation | V^2 = 3KT/m |
Thermal Stress | O (stress) = ∂∆TE |
Calibrating Thermometers | Tx = X - Xo / X100 - Xo |
Pressure - Density Equation | P = ∫g∆h + Patm |
Resistance Thermometers | R = Ro (1 + ∂T + ßT^2) |
Calorimeter Equation | ∆U = MC(T2 - T1) + (MC(T2-T1) ^ ^ ^ (MC(T2-T1)) WATER CALORIMETER |
Linear Expansions of Solids | ∆L = L[1 + ∂(T2 - T1)] |
Work equation relating to pv | ∆W = P∆V |
Vertical Deflection Equation (AND DERIVATION) | ∆h = L∂ ∂ = †/ß ∆h = L†/ß ∂ is shear strain † is shear stress ß is shear modulus |
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