/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 12 What form does the energy balanc... [FREE SOLUTION] | 91Ó°ÊÓ

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What form does the energy balance take for an isolated system?

Short Answer

Expert verified
The energy balance for an isolated system is \(\frac{dE}{dt} = 0\), meaning the internal energy remains constant.

Step by step solution

01

Understand an Isolated System

An isolated system is a system that does not exchange matter or energy with its surroundings. It is completely self-contained.
02

Review the First Law of Thermodynamics

The first law of thermodynamics states that energy cannot be created or destroyed, only transferred or converted from one form to another. Mathematically, it is expressed as \(\frac{dE}{dt} = Q - W\), where \(E\) is the internal energy, \(Q\) is the heat added to the system, and \(W\) is the work done by the system.
03

Apply the Concept to an Isolated System

For an isolated system, there is no exchange of energy with the surroundings. This means that heat \(Q = 0\) and work \(W = 0\).
04

Derive the Energy Balance Equation

Given that \(Q = 0\) and \(W = 0\), the energy balance equation simplifies to: \(\frac{dE}{dt} = 0\). Therefore, the internal energy \(E\) of an isolated system remains constant over time.

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Key Concepts

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

isolated system
An isolated system is a crucial idea in thermodynamics. It helps us understand certain behaviors in physics and chemistry.
In simple terms, an isolated system does not interact with its surroundings. This means no matter or energy can enter or exit the system.
Think of it like a perfectly sealed box, where nothing comes in or goes out.
This isolation can be conceptual, as in a thought experiment, or somewhat physical, like an insulated container. However, true isolated systems are rare in real life; most systems interact with their environment in some way. This concept is foundational in theoretical studies.
By understanding isolated systems, we can analyze how internal energy behaves without external interference.
first law of thermodynamics
The first law of thermodynamics is one of the fundamental principles governing energy in physics. It's often summed up as the principle of energy conservation.
This law tells us that energy cannot be created or destroyed. Instead, it can only change forms. For instance, chemical energy can become heat energy, or mechanical energy can become electrical energy.
The mathematical form of this law is given by \(\frac{dE}{dt} = Q - W\), where \(E\) is the internal energy, \(Q\) is the heat added to the system, and \(W\) is the work done by the system.
This equation leads to the understanding that any change in internal energy is due to heat transferred to the system or work done by the system. When applying this principle to different scenarios, we can better grasp how energy flows and transforms.
energy conservation
Energy conservation in an isolated system has an interesting outcome. Since the system does not interact with its surroundings, both heat transfer and work are zero.
Therefore, by the first law of thermodynamics, \(Q = 0\) and \(W = 0\). When substituted into the energy balance equation, we get \(\frac{dE}{dt} = 0\).
This simplification means the internal energy remains constant over time, as no energy is added or removed. It's a straightforward and significant result because it illustrates energy conservation in its purest form.
Recognizing this helps in many areas of science, from analyzing closed systems in laboratories to large-scale natural processes. This understanding forms the basis for deeper studies into more complex thermodynamic systems.
Thus, grasping these fundamental principles creates a strong foundation for mastering thermodynamics.

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Most popular questions from this chapter

A heat pump cycle delivers energy by heat transfer to a dwelling at a rate of \(63,300 \mathrm{~kJ} / \mathrm{h}\). The power input to the cycle is \(5.82 \mathrm{~kW}\) (a) Determine the coefficient of performance of the cycle. (b) Evaluating electricity at \(\$ 0.08\) per \(\mathrm{kW} \cdot \mathrm{h}\), determine the cost of electricity in a month when the heat pump operates for 200 hours.

\(.\) In a rigid insulated container of volume \(0.8 \mathrm{~m}^{3}, 2.5 \mathrm{~kg}\) of air is filled. A paddle wheel is fitted in the container and it transfers energy to the contained air at a constant rate of \(12 \mathrm{~W}\) for a period of \(1 \mathrm{~h}\). There is no change in the potential or kinetic energy of the system. Determine the energy transfer by the wheel to the air per \(\mathrm{kg}\) of air.

The drag force, \(F_{\mathrm{d}}\), imposed by the surrounding air on a vehicle moving with velocity \(\mathrm{V}\) is given by $$ F_{\mathrm{d}}=C_{\mathrm{d}} \mathrm{A}_{2}^{\frac{1}{2} \rho} \mathrm{V}^{2} $$ where \(C_{\mathrm{d}}\) is a constant called the drag coefficient, \(\mathrm{A}\) is the projected frontal area of the vehicle, and \(\rho\) is the air density. Determine the power, in \(\mathrm{kW}\), required to overcome aerodynamic drag for a truck moving at \(110 \mathrm{~km} / \mathrm{h}\), if \(C_{\mathrm{d}}=0.65, \mathrm{~A}=10 \mathrm{~m}^{2}\), and \(\rho=1.1 \mathrm{~kg} / \mathrm{m}^{3}\).

An air-conditioning unit with a coefficient of performance of \(2.93\) provides \(5,275 \mathrm{~kJ} / \mathrm{h}\) of cooling while operating during the cooling season 8 hours per day for 125 days. If you pay 10 cents per \(\mathrm{kW} \cdot \mathrm{h}\) for electricity, determine the cost, in, dollars, for the cooling season.

\(.\) A block of mass \(10 \mathrm{~kg}\) moves along a surface inclined \(30^{\circ}\) relative to the horizontal. The center of gravity of the block. is elevated by \(3.0 \mathrm{~m}\) and the kinetic energy of the block decreases by \(50 \mathrm{~J}\). The block is acted upon by a constant force \(\mathbf{R}\) parallel to the incline, and by the force of gravity. Assume frictionless surfaces and let \(g=9.81 \mathrm{~m} / \mathrm{s}^{2}\). Determine the magnitude and direction of the constant force \(\mathbf{R}\), in \(\mathrm{N}\).

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