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Define energy, kinetic energy, potential energy, and internal energy.

Short Answer

Expert verified
Energy is the capacity to do work. Kinetic energy is due to motion; potential energy is due to position. Internal energy is the total energy within a system.

Step by step solution

01

Define Energy

Energy is the capacity to do work or produce change. It is a fundamental concept in physics and exists in various forms. Energy cannot be created or destroyed; it can only be transformed from one form to another. This principle is known as the law of conservation of energy.
02

Define Kinetic Energy

Kinetic energy is the energy possessed by an object due to its motion. The formula to calculate the kinetic energy of an object is given by \( KE = \frac{1}{2}mv^2 \), where \( m \) is the mass of the object and \( v \) is its velocity. Kinetic energy depends on both mass and speed of the object.
03

Define Potential Energy

Potential energy is the energy stored in an object due to its position in a force field, such as a gravitational field. A common type of potential energy is gravitational potential energy, which is calculated as \( PE = mgh \), where \( m \) is mass, \( g \) is the acceleration due to gravity, and \( h \) is the height above a reference point.
04

Define Internal Energy

Internal energy is the total energy contained within a system due to the random motion of particles and the potential energy associated with intermolecular forces. It includes both the kinetic energy of particles and the potential energy of their interactions. Internal energy is a state function, important in thermodynamics.

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Key Concepts

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

Kinetic Energy
Kinetic energy is an essential concept in physics that describes the energy an object possesses due to its motion. Imagine a rolling ball or a flying airplane; both have kinetic energy because they are moving. This kind of energy depends on two important factors: mass and velocity. To calculate kinetic energy, we use the formula: \[ KE = \frac{1}{2}mv^2 \] where
  • \( m \) is the mass of the object in kilograms (kg), and
  • \( v \) is the velocity of the object in meters per second (m/s).
The faster an object moves, or the heavier it is, the more kinetic energy it has. It's important to remember that if an object is not moving, its kinetic energy is zero, because velocity is a key part of the equation.
Potential Energy
Potential energy is the energy stored within an object due to its position or state. This type of energy gives an object the potential to do work in the future. One common example is a book placed on a high shelf. It has gravitational potential energy because of its position in the Earth’s gravitational field. The gravitational potential energy can be calculated using the formula: \[ PE = mgh \] where
  • \( m \) is the mass in kilograms,
  • \( g \) is the acceleration due to gravity (9.8 m/s² on Earth), and
  • \( h \) is the height in meters above a reference point, usually ground level.
Remember that potential energy is not just about height. It can also be due to the arrangement of atoms within a molecule or the compression of a spring. All these scenarios involve an object or system having stored energy, ready to be converted into other forms, like kinetic energy.
Internal Energy
Internal energy is a concept primarily used in the study of thermodynamics. It refers to the total energy contained within a system, which results from the random motion of its particles and the interactions between them. When you consider internal energy, think about everything inside a container—like a pot of boiling water. Inside, molecules are moving, colliding, and interacting with each other. This movement and interaction create what we call internal energy. It includes two main components:
  • The kinetic energy due to the motion of molecules, and
  • The potential energy from the forces between molecules.
Unlike kinetic and potential energy, internal energy is a state function. It does not change unless the system’s temperature, volume, or energy exchange (like heat) changes. Internal energy is critical when discussing the heat, work, and energy exchange in thermodynamics.
Conservation of Energy
The principle of conservation of energy is a fundamental concept that states energy cannot be created or destroyed. Instead, it can only be transformed or transferred from one form to another. This principle is the backbone of many scientific laws and principles across different fields. In essence, when energy is used to move an object, like a swinging pendulum, it might start as potential energy at the highest point. As it swings down, that energy converts to kinetic energy. Throughout this motion, the total energy remains constant, unless it is acted upon by an external force like friction or air resistance. In real-world situations, energy conservation helps us understand everything from the efficiency of machines to the balance of natural systems. By ensuring that energy is conserved in all processes, scientists and engineers can design more sustainable systems and solutions.

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Most popular questions from this chapter

A 19.6-g sample of a metal was heated to \(61.67^{\circ} \mathrm{C}\). When the metal was placed into \(26.7 \mathrm{~g}\) of water in a calorimeter, the temperature of the water increased from \(25.00^{\circ} \mathrm{C}\) to \(30.00^{\circ} \mathrm{C}\). What is the specific heat of the metal?

Part 1: In an insulated container, you mix 200. g of water at \(80^{\circ} \mathrm{C}\) with \(100 . \mathrm{g}\) of water at \(20^{\circ} \mathrm{C}\). After mixing, the temperature of the water is \(60^{\circ} \mathrm{C}\). a. How much did the temperature of the hot water change? How much did the temperature of the cold water change? Compare the magnitudes (positive values) of these changes. b. During the mixing, how did the heat transfer occur: from hot water to cold, or from cold water to hot? C. What quantity of heat was transferred from one sample to the other? d. How does the quantity of heat transferred to or from the hot-water sample compare with the quantity of heat transferred to or from the cold-water sample? e. Knowing these relative quantities of heat, why is the temperature change of the cold water greater than the magnitude of the temperature change of the hot water. f. A sample of hot water is mixed with a sample of cold water that has twice its mass. Predict the temperature change of each of the samples. g. You mix two samples of water, and one increases by \(20^{\circ} \mathrm{C}\), while the other drops by \(60^{\circ} \mathrm{C}\). Which of the samples has less mass? How do the masses of the two water samples compare? h. A 7 -g sample of hot water is mixed with a \(3-\mathrm{g}\) sample of cold water. How do the temperature changes of the two water samples compare? Part \(2:\) A sample of water is heated from \(10^{\circ} \mathrm{C}\) to \(50^{\circ} \mathrm{C}\). Can you calculate the amount of heat added to the water sample that caused this temperature change? If not, what information do you need to perform this calculation? Part 3: Two samples of water are heated from \(20^{\circ} \mathrm{C}\) to \(60^{\circ} \mathrm{C}\). One of the samples requires twice as much heat to bring about this temperature change as the other. How do the masses of the two water samples compare? Explain your reasoning.

When steam condenses to liquid water, \(2.26 \mathrm{~kJ}\) of heat is released per gram. The heat from \(168 \mathrm{~g}\) of steam is used to heat a room containing \(6.44 \times 10^{4} \mathrm{~g}\) of air \((20 \mathrm{ft} \times 12 \mathrm{ft} \times 8 \mathrm{ft})\). The specific heat of air at normal pressure is \(1.015 \mathrm{~J} /\left(\mathrm{g} \cdot{ }^{\circ} \mathrm{C}\right) .\) What is the change in air temperature, assuming the heat from the steam is all absorbed by air?

Colorless nitric oxide, NO, combines with oxygen to form nitrogen dioxide, \(\mathrm{NO}_{2}\), a brown gas. $$ 2 \mathrm{NO}(g)+\mathrm{O}_{2}(g) \longrightarrow 2 \mathrm{NO}_{2}(g) ; \Delta H=-114 \mathrm{~kJ} $$ What is the enthalpy change per gram of nitric oxide?

Is the following reaction the appropriate one to use in determining the enthalpy of formation of methane, \(\mathrm{CH}_{4}(g) ?\) Why or why not? $$ \mathrm{C}(g)+4 \mathrm{H}(g) \longrightarrow \mathrm{CH}_{4}(g) $$

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