Q = U + Wwhere, Q = heat supplied. U = 0 = Internal energy, W = work doneSo, the heat transfer equation is, Q = W = 100 kW ProcessWork DoneConstant Pressure (Isobaric / Isopiestic)W1-2 = P(V2 – V1)Constant Volume (Isochoric)W1-2 = 0Isothermal\({W_{1 - 2}} = {p_1}{V_1}\ln \left( {\FRAC{{{p_1}}}{{{p_2}}}} \RIGHT) = {p_2}{V_2}\ln \left( {\frac{{{p_1}}}{{{p_2}}}} \right)\)PolytropicFor Adiabatic (n = γ = 1.4)\({W_{1 - 2}} = \frac{{{p_1}{V_1} - {p_2}{V_2}}}{{n - 1}} = \frac{{{p_1}{V_1}}}{{n - 1}}\left[ {1 - {{\left( {\frac{{{p_2}}}{{{p_1}}}} \right)}^{\frac{{n - 1}}{n}}}} \right]\)

"> Q = U + Wwhere, Q = heat supplied. U = 0 = Internal energy, W = work doneSo, the heat transfer equation is, Q = W = 100 kW ProcessWork DoneConstant Pressure (Isobaric / Isopiestic)W1-2 = P(V2 – V1)Constant Volume (Isochoric)W1-2 = 0Isothermal\({W_{1 - 2}} = {p_1}{V_1}\ln \left( {\FRAC{{{p_1}}}{{{p_2}}}} \RIGHT) = {p_2}{V_2}\ln \left( {\frac{{{p_1}}}{{{p_2}}}} \right)\)PolytropicFor Adiabatic (n = γ = 1.4)\({W_{1 - 2}} = \frac{{{p_1}{V_1} - {p_2}{V_2}}}{{n - 1}} = \frac{{{p_1}{V_1}}}{{n - 1}}\left[ {1 - {{\left( {\frac{{{p_2}}}{{{p_1}}}} \right)}^{\frac{{n - 1}}{n}}}} \right]\)

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In a reversible isothermal expansion process fluid expands from 10 bar and 2 m3 to 2 bar and 10 m3. During the process the heat supplied is at the rate of 100 kW. What is the rate of work done during the process

Fluid Mechanics First Law Thermodynamics in Fluid Mechanics . 8 months ago

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Explanation:Heat transfer in the constant temperature process by first law of thermodynamics is given as:Q = U + Wwhere, Q = heat supplied. U = 0 = Internal energy, W = work doneSo, the heat transfer equation is, Q = W = 100 kW ProcessWork DoneConstant Pressure (Isobaric / Isopiestic)W1-2 = P(V2 – V1)Constant Volume (Isochoric)W1-2 = 0Isothermal\({W_{1 - 2}} = {p_1}{V_1}\ln \left( {\FRAC{{{p_1}}}{{{p_2}}}} \RIGHT) = {p_2}{V_2}\ln \left( {\frac{{{p_1}}}{{{p_2}}}} \right)\)PolytropicFor Adiabatic (n = γ = 1.4)\({W_{1 - 2}} = \frac{{{p_1}{V_1} - {p_2}{V_2}}}{{n - 1}} = \frac{{{p_1}{V_1}}}{{n - 1}}\left[ {1 - {{\left( {\frac{{{p_2}}}{{{p_1}}}} \right)}^{\frac{{n - 1}}{n}}}} \right]\)

Posted on 12 Nov 2024, this text provides information on Fluid Mechanics related to First Law Thermodynamics in Fluid Mechanics. Please note that while accuracy is prioritized, the data presented might not be entirely correct or up-to-date. This information is offered for general knowledge and informational purposes only, and should not be considered as a substitute for professional advice.

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