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(a) Write an equation that expresses the first law of thermodynamics in terms of heat and work. (b) Under what condi. tions will the quantities \(q\) and \(w\) be negative numbers?

Short Answer

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(a) \( \Delta U = q + w \); (b) \( q \) is negative when heat is released, and \( w \) is negative when work is done by the system.

Step by step solution

01

Understanding the First Law of Thermodynamics

The first law of thermodynamics is a statement of the conservation of energy. It states that energy can neither be created nor destroyed, only transformed from one form to another. In terms of internal energy, heat, and work, this law can be expressed using an equation.
02

Expressing the First Law in an Equation

The equation that represents the first law of thermodynamics in terms of internal energy change, heat, and work is given by: \( \Delta U = q + w \), where \( \Delta U \) is the change in internal energy of the system, \( q \) is the heat added to the system, and \( w \) is the work done on the system.
03

Understanding When \( q \) is Negative

The quantity \( q \) is negative when heat is released from the system to the surroundings. This often occurs in exothermic processes, where the system loses heat as it transforms energy into work or other forms.
04

Understanding When \( w \) is Negative

The quantity \( w \) is negative when work is done by the system on its surroundings. This typically occurs when the system expands, such as in the case of an expanding gas pushing against a piston.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

First Law of Thermodynamics
The first law of thermodynamics is a fundamental principle, pivotal in understanding energy interactions in physical systems. It asserts that energy cannot be created or destroyed; it can only change forms. In simpler terms, this law emphasizes the continuous balance of energy. When energy enters or leaves a system, it does so either as heat or as work. This conservation principle can be represented using an equation: \[ \Delta U = q + w \]Here, \( \Delta U \) represents the change in internal energy of the system, \( q \) denotes heat added to the system, and \( w \) is work done on the system. This equation ties together internal energy, heat, and external work, providing a complete account of energy transformations.
Conservation of Energy
Conservation of energy is the underlying theme of the first law of thermodynamics. It dictates that the total energy of an isolated system remains constant. In practical scenarios:
  • Energy can be transferred between a system and its surroundings.
  • It can change forms, but the total energy count never changes.
The conservation of energy ensures that any energy "lost" by a system is "gained" by its surroundings, and vice versa. This balancing act is crucial in processes like chemical reactions, engine operations, and even biological metabolism.
Internal Energy
Internal energy encompasses all the energy contained within a system. It includes kinetic energies of particles, potential energy in chemical bonds, and more. As a dynamic component:
  • Internal energy changes when heat is transferred in or out of a system (heat, \( q \)).
  • It also changes when work is performed by or on the system (work, \( w \)).
The internal energy change is central to understanding how energy transactions occur within a system, reflected in the equation \( \Delta U = q + w \). By observing changes in internal energy, one can infer whether a system is gaining or losing energy.
Heat and Work
Heat and work are the two primary mechanisms through which energy is exchanged between a system and its surroundings. They play distinctive roles:- **Heat (\( q \))**: - Represents energy transfer due to temperature difference. - Is positive when heat enters the system. - Is negative when the system releases heat (e.g., during cooling processes).- **Work (\( w \))**: - Occurs when forces act over distances, changing the system's energy. - Is positive when work is done on the system. - Is negative when the system performs work on its surroundings (e.g., gas expansion pushing a piston).Together, heat and work explain the flow and transformation of energy within thermodynamic systems. Recognizing whether these values are negative or positive helps determine the direction and impact of energy changes.

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Most popular questions from this chapter

From the enthalpies of reaction $$ 2 \mathrm{C}(s)+\mathrm{O}_{2}(g) \longrightarrow 2 \mathrm{CO}(g) \quad \Delta H=-221.0 \mathrm{~kJ} $$ \(2 \mathrm{C}(s)+\mathrm{O}_{2}(g)+4 \mathrm{H}_{2}(g) \longrightarrow 2 \mathrm{CH}_{3} \mathrm{OH}(g) \quad \Delta H=-402.4 \mathrm{~kJ}\) calculate \(\Delta H\) for the reaction $$ \mathrm{CO}(g)+2 \mathrm{H}_{2}(\mathrm{~g}) \longrightarrow \mathrm{CH}_{3} \mathrm{OH}(g) $$

Identify the force present and explain whether work is done when (a) an electron moves in a circle at a fixed distance from a proton, \((\mathbf{b})\) an iron nail is attracted by and pulled onto a magnet.

The standard enthalpies of formation of gaseous propyne \(\left(\mathrm{C}_{3} \mathrm{H}_{4}\right)\), propylene \(\left(\mathrm{C}_{3} \mathrm{H}_{6}\right)\), and propane \(\left(\mathrm{C}_{3} \mathrm{H}_{8}\right)\) are \(+185.4,+20.4,\) and \(-103.8 \mathrm{~kJ} / \mathrm{mol}\), respectively. (a) Calculate the heat evolved per mole on combustion of each substance to yield \(\mathrm{CO}_{2}(g)\) and \(\mathrm{H}_{2} \mathrm{O}(g) .\) (b) Calculate the heat evolved on combustion of \(1 \mathrm{~kg}\) of each substance. \((\mathbf{c})\) Which is the most efficient fuel in terms of heat evolved per unit mass?

At one time, a common means of forming small quantities of oxygen gas in the laboratory was to heat \(\mathrm{KClO}_{3}:\) $$ 2 \mathrm{KClO}_{3}(s) \longrightarrow 2 \mathrm{KCl}(s)+3 \mathrm{O}_{2}(g) \quad \Delta H=-89.4 \mathrm{~kJ} $$ For this reaction, calculate \(\Delta H\) for the formation of (a) \(1.36 \mathrm{~mol}\) of \(\mathrm{O}_{2}\) and \((\mathbf{b}) 10.4 \mathrm{~g}\) of \(\mathrm{KCl}\). (c) The decomposition of \(\mathrm{KClO}_{3}\) proceeds spontaneously when it is heated. Do you think that the reverse reaction, the formation of \(\mathrm{KClO}_{3}\) from \(\mathrm{KCl}\) and \(\mathrm{O}_{2}\), is likely to be feasible under ordinary conditions? Explain your answer.

It is estimated that the net amount of carbon dioxide fixed by photosynthesis on the landmass of Earth is \(5.5 \times 10^{16} \mathrm{~g} / \mathrm{yr}\) of \(\mathrm{CO}_{2}\). Assume that all this carbon is converted into glucose. (a) Calculate the energy stored by photosynthesis on land per year, in \(\mathrm{kJ} .\) (b) Calculate the average rate of conversion of solar energy into plant energy in megawatts, MW \((1 \mathrm{~W}=1 \mathrm{~J} / \mathrm{s})\). A large nuclear power plant produces about \(10^{3} \mathrm{MW}\). The energy of how many such nuclear power plants is equivalent to the solar energy conversion?

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