Heat, Work & Thermodynamics First Law

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Questions and Answers

For an isobaric process, which of the following statements correctly describes the relationship between work (W), pressure (p), and volume change (V₂ - V₁)?

  • W = V₂ - V₁
  • W = p / (V₂ - V₁)
  • W = pV₁V₂
  • W = p(V₂ - V₁) (correct)

During an adiabatic process, what condition holds true regarding heat transfer (Q) between the system and its surroundings?

  • Q is infinite, indicating instantaneous heat transfer.
  • Q < 0, indicating heat is removed from the system.
  • Q = 0, indicating no heat transfer. (correct)
  • Q > 0, indicating heat is added to the system.

A thermodynamic system undergoes a process where its internal energy remains constant. Which of the following statements must be true about this process?

  • The work done by the system is greater than the heat added to it.
  • The system performs work equal to the heat added to it. (correct)
  • No work is done by or on the system.
  • The heat added to the system is zero.

For an ideal gas, under what condition does the internal energy depend only on its temperature?

<p>Regardless of pressure or volume. (D)</p> Signup and view all the answers

Which type of thermodynamic process is characterized by a constant volume?

<p>Isochoric (C)</p> Signup and view all the answers

If a system absorbs 150 J of heat and performs 100 J of work, what is the change in internal energy of the system?

<p>50 J (B)</p> Signup and view all the answers

In adiabatic processes involving ideal gases, which of the following quantities remains constant?

<p>$TV^{\gamma-1}$ (A)</p> Signup and view all the answers

What does a negative value of work (W) indicate in a thermodynamic process?

<p>Work is done <em>on</em> the system. (A)</p> Signup and view all the answers

What is the relationship between molar heat capacities at constant pressure ($C_p$) and constant volume ($C_v$) for an ideal gas, in terms of the ideal gas constant (R)?

<p>$C_p - C_v = R$ (D)</p> Signup and view all the answers

Consider a thermodynamic process. The heat added to the system and the work done by the system depend on:

<p>The path taken between the initial and final states. (C)</p> Signup and view all the answers

Flashcards

Thermodynamic Processes

A thermodynamic system's potential to exchange energy with its surroundings.

1st Law of Thermodynamics

The heat added equals the change in internal energy plus work done.

Adiabatic Process

No heat exchange occurs.

Isochoric Process

Constant volume.

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Isobaric Process

Constant pressure.

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Isothermal Process

Constant temperature.

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Ideal Gas Internal Energy

Internal energy depends only on temperature, not pressure or volume

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Adiabatic ideal gas process

TV^(γ-1) and pV^γ are constant.

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Work in Thermodynamics

The amount of work done by the system.

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Internal Energy (U)

The energy stored within a system.

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Study Notes

Heat and Work in Thermodynamic Processes

  • A thermodynamic system can exchange energy with its surroundings through heat transfer or mechanical work.
  • When a system's volume changes from V₁ to V₂ at pressure p, the work W is the integral of p with respect to volume: W = ∫(from V₁ to V₂) pdV.
  • For constant pressure, work done equals pressure times the change in volume: W = p(V₂ - V₁).
  • A negative W indicates work done on the system.
  • Heat added to the system and work done depend on the initial and final states and the path of intermediate states.

First Law of Thermodynamics

  • The first law states that when heat Q is added to a system, and the system does work W, internal energy U changes by Q - W: ΔU = Q - W.
  • This also applies to infinitesimal processes: dU = dQ - dW.
  • Internal energy depends only on the system's state and the change in internal energy in a process depends on initial and final states, not the path.
  • The internal energy of an isolated system remains constant.

Important Kinds of Thermodynamic Processes

  • Adiabatic: No heat transfer (Q = 0).
  • Isochoric: Constant volume, no work done (W = 0).
  • Isobaric: Constant pressure, work done is W = p(V₂ - V₁).
  • Isothermal: Constant temperature.

Thermodynamics of Ideal Gases

  • Internal energy depends only on temperature, not pressure or volume.
  • For other substances, internal energy depends on both pressure and temperature.
  • Molar heat capacities Cₚ and Cᵥ of an ideal gas differ by R (ideal-gas constant): Cₚ = Cᵥ + R.
  • The dimensionless ratio of heat capacities, Cₚ/Cᵥ, is denoted by γ: γ = Cₚ/Cᵥ.

Adiabatic Processes in Ideal Gases

  • For an adiabatic process with an ideal gas, TV^(γ-1) and pV^γ are constant.
  • Work done by an ideal gas during adiabatic expansion can be expressed in terms of initial and final temperatures: W = nCᵥ(T₁ - T₂).
  • Work can also be expressed with initial and final values of pressure and volume: W = (Cᵥ/R)(p₁V₁ - p₂V₂) = (1/(γ-1))(p₁V₁ - p₂V₂).

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