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What is internal energy?

Short Answer

Expert verified
Internal energy is the total energy within a system, including both kinetic and potential energies of all particles.

Step by step solution

01

Define Internal Energy

Internal energy is the total energy contained within a thermodynamic system. It includes all microscopic kinetic and potential energies.
02

Understand Components

Internal energy consists of various components such as the kinetic energy due to the motion of particles, and potential energy from interactions between particles.
03

Relate to Thermodynamics

In thermodynamics, internal energy is often denoted by the symbol \(U\), and it changes when heat or work is added to or removed from the system.
04

Use the First Law of Thermodynamics

According to the First Law of Thermodynamics, the change in internal energy \(\Delta U\) of a system is equal to the heat \(Q\) added to the system minus the work \(W\) done by the system: \(\Delta U = Q - W\).
05

Connect to Everyday Context

In everyday terms, when you heat a system or compress it, its internal energy changes by affecting particle motion and potential energy.

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Key Concepts

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

Thermodynamic System
A thermodynamic system is a specific part of the universe that we are interested in studying. Everything outside this system is known as the surroundings. We often examine how energy moves into or out of this well-defined region to understand the system's behavior better.

Thermodynamic systems can be classified in a few different ways, depending on what energies or substances can pass through its boundaries. Common types include:
  • Closed System: Only energy, such as heat or work, can cross the boundary, but not matter. An example is a sealed container of gas.
  • Open System: Both energy and matter can leave or enter. A boiling pot of water without a lid is a practical example.
  • Isolated System: Neither matter nor energy can penetrate the boundary. Examples are very rare in the real world but could include a perfectly insulated container.
By understanding a system's type, we can predict how it might behave or change under different conditions, especially when applying thermodynamic principles.
First Law of Thermodynamics
The First Law of Thermodynamics is all about energy conservation. It tells us that energy cannot be created or destroyed in an isolated system. Instead, it is transformed from one form to another.

Mathematically, this law is expressed as:\[ \Delta U = Q - W \]Here, \( \Delta U \) represents the change in internal energy of a system, \( Q \) is the heat added to the system, and \( W \) is the work done by the system.

In simpler terms, if you add heat to the system (increasing \( Q \)), or if the system does work on its surroundings (increasing \( W \)), the internal energy of the system will change. This fundamental principle helps us understand how systems exchange energy and gives us a way to predict energy changes under various conditions.
Heat and Work Interaction
Heat and work are two primary forms of energy transfer within a thermodynamic system. Understanding their interaction is essential for grasping how internal energy changes occur.

Heat: This is the energy transferred due to temperature difference between a system and its surroundings. When heat is added to a system, it can increase the system's internal energy as the particles move more vigorously.

Work: This refers to the energy transfer that occurs when an external force acts on the system, often changing its volume. Compressions or expansions that move pistons are classic examples.

In thermodynamics, the balance of heat and work interactions influences the system's internal state. For instance, heating a gas inside a piston can do work by pushing the piston upwards. This reduces the available internal energy because part of it is used to perform the work. Understanding how heat and work contribute to energy transformations is vital in fields ranging from engineering to environmental science.

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Most popular questions from this chapter

Which has more kinetic energy, a \(1400-\mathrm{kg}\) car moving at \(115 \mathrm{~km} / \mathrm{h}\) or a \(12,000-\mathrm{kg}\) truck moving at \(38 \mathrm{~km} / \mathrm{h} ?\)

Used in welding metals, the reaction of acetylene with oxygen has $$\begin{aligned}\Delta H^{\circ}=&-1256.2 \mathrm{~kJ}: \\ \mathrm{C}_{2} \mathrm{H}_{2}(\mathrm{~g})+5 / 2 \mathrm{O}_{2}(g) \longrightarrow \mathrm{H}_{2} \mathrm{O}(g)+2 \mathrm{CO}_{2}(g) \\ \Delta H^{\circ}=-1256.2 \mathrm{~kJ}\end{aligned}$$ How much \(P V\) work is done in kilojoules and what is the value of \(\Delta E\) in kilojoules for the reaction of \(6.50 \mathrm{~g}\) of acetylene at atmospheric pressure if the volume change is \(-2.80 \mathrm{~L}\) ?

Calculate the work done in joules by a chemical reaction if the volume increases from \(3.2 \mathrm{~L}\) to \(3.4 \mathrm{~L}\) against a constant external pressure of \(3.6 \mathrm{~atm}\). What is the sign of the energy change?

(a) When \(0.350 \mathrm{~g}\) of biodiesel \(\left(\mathrm{C}_{19} \mathrm{H}_{38} \mathrm{O}_{2}\right)\) is burned in a bomb calorimeter, the temperature of both the water and the calorimeter rise in temperature by \(6.85^{\circ} \mathrm{C}\). Assuming that the bath contains \(300.0 \mathrm{~g}\) of water and that the heat capacity for the calorimeter is \(675 \mathrm{~J} /{ }^{\circ} \mathrm{C}\), calculate combustion en\(\operatorname{ergy}(\Delta E)\) for biodiesel in units of \(\mathrm{k} \mathrm{J} / \mathrm{g}\) (b) Calculate combustion energy \((\Delta E)\) for biodiesel in units of \(\mathrm{kJ} / \mathrm{mol}\) (c) If the density of biodiesel is \(0.880 \mathrm{~g} / \mathrm{mL}\), calculate combustion energy \((\Delta E)\) for biodiesel in units of \(\mathrm{kJ} / \mathrm{mL}\).

Tell whether the entropy changes, \(\Delta S\), for the following processes are likely to be positive or negative: (a) The conversion of liquid water to water vapor at \(100^{\circ} \mathrm{C}\) (b) The freezing of liquid water to ice at \(0{ }^{\circ} \mathrm{C}\) (c) The eroding of a mountain by a glacier

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