
The first law of thermodynamics, also known as the law of conservation of energy, states that energy cannot be created or destroyed, but it can be converted from one form to another. This law is a fundamental principle in thermodynamics, which is a discipline that studies the interaction of heat and other types of energy, as well as the role of temperature, volume, and pressure in energy exchange. The first explicit statement of the first law of thermodynamics was made by Rudolf Clausius in 1850, but the law has since been refined and built upon by various scientists over the years. The law is based on the concept of internal energy and its relationship to temperature and work, and it helps to explain the behaviour of systems in thermodynamic processes.
| Characteristics | Values |
|---|---|
| Date of formulation | 1850 |
| Formulation credited to | Rudolf Clausius |
| Other contributors | Germain Hess, Julius Robert von Mayer, James Prescott Joule, Hermann von Helmholtz, William Thomson, Sadi Carnot, Walther Nernst |
| Other names | Law of conservation of energy, conservation of energy |
| Equation | ΔU = Q – W |
| Description | Energy is conserved, it cannot be created or destroyed but can be converted between different forms |
| Scope | Applicable to thermodynamic processes, closed systems, the universe |
| Perpetual motion machines | Prohibits perpetual motion machines of the first kind |
| Internal energy | The internal energy of a system increases when heat increases or when work is done on the system |
| Energy transfer | Energy can be transferred between systems with or without the transfer of matter |
| Energy in the universe | The total amount of energy in the universe is constant |
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What You'll Learn

The first law of thermodynamics is a version of the law of conservation of energy
The first law of thermodynamics is generally thought to be the least demanding to grasp, as it is an extension of the law of conservation of energy, meaning that energy can be neither created nor destroyed. The first law of thermodynamics states that the total energy of a system remains constant, even if it is converted from one form to another. This is also referred to as the conservation of energy principle, meaning that energy can neither be created nor destroyed but rather transformed into various forms as the fluid within the control volume changes. The first law of thermodynamics allows for many possible states of a system to exist. However, experience indicates that only certain states occur.
The first law of thermodynamics evolved from the experimental demonstration that heat and mechanical work are interchangeable forms of energy. The first law of thermodynamics is adapted for thermodynamic processes. In general, the conservation law states that the total energy of an isolated system is constant; energy can be transformed from one form to another, but it can be neither created nor destroyed. The first law of thermodynamics is also important in understanding the concept of internal energy and its relationship to temperature. If a system has a definite temperature, then its total energy has three distinguishable components: kinetic energy, potential energy, and internal energy.
The first law of thermodynamics is also related to the concept of work from a thermodynamics point of view. Work is a process of transferring energy to or from a system in ways that can be described by macroscopic mechanical forces acting between the system and its surroundings. The work done by the system can come from its overall kinetic energy, from its overall potential energy, or from its internal energy. The first law of thermodynamics also helps to clarify the meaning of temperature and its empirical definition.
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Energy can be converted from one form to another
The first law of thermodynamics is a proven principle in physics, stating that energy is conserved and cannot be created or destroyed. This law, also known as the law of conservation of energy, highlights that energy can only be transformed or converted from one form to another.
Energy conversion, also known as energy transformation, is the process of changing energy from one form to another. This principle is fundamental to our understanding of physics and the behaviour of energy. It is important to note that while energy can be converted, it can also be transferred to different locations or objects without changing its form.
There are numerous examples of energy conversion that occur in everyday life. One common example is the conversion of kinetic energy to thermal energy. When a moving object, such as a car, comes to a stop, the kinetic energy it had while in motion is transformed into thermal energy (heat) due to the friction between the tires and the road. This example illustrates how energy is neither created nor destroyed but simply changes form.
Another example of energy conversion is observed in the operation of a combustion engine. In this case, the chemical energy stored in the fuel is converted into thermal energy through the process of combustion. This thermal energy then undergoes further conversion into mechanical energy, showcasing how energy can transform through multiple forms.
Additionally, the concept of energy conversion is evident in natural processes. For instance, starlight from the Sun can be captured and stored as gravitational potential energy on Earth. This occurs in natural phenomena like avalanches or the evaporation of water from oceans, which subsequently leads to the formation of precipitation at higher altitudes. The energy stored in these elevated positions can then be harnessed to generate electricity through hydroelectric dams.
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Energy cannot be created or destroyed
The first law of thermodynamics, also known as the law of conservation of energy, states that energy cannot be created or destroyed. This means that the total energy in a closed system remains constant, even if it is converted from one form to another. For example, kinetic energy—the energy an object possesses when in motion—is converted to heat energy when a driver presses the brakes to slow down a car.
The first law of thermodynamics was formulated in the 19th century, with early contributions from scientists such as Hermann von Helmholtz, Germain Hess, and Rudolf Clausius. The first explicit statement of the law was made by Clausius in 1850, referring to cyclic thermodynamic processes and the existence of a function of state of the system, the internal energy. The law distinguishes two principal forms of energy transfer: heat and thermodynamic work.
The law also defines the internal energy of a system, which is an extensive property that accounts for the balance of heat transfer, thermodynamic work, and matter transfer into and out of the system. The internal energy of a system can decrease if the system gives off heat or does work, and it can increase if heat or work is done on the system. This change in internal energy is described by the equation ΔU = q + w, where ΔU is the change in internal energy, q is the heat added or removed from the system, and w is the work done on or by the system.
The first law of thermodynamics is fundamental to understanding any thermodynamic process or calculation. It also has implications for the design and control of such processes, as well as for process improvement and optimization. The law also prohibits the existence of perpetual motion machines of the first kind, which would produce work without any energy input.
The concept of energy conservation stated by the first law of thermodynamics has profound implications for our understanding of the universe. It suggests that the total energy of the universe has remained constant since the beginning, and will continue to do so.
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The internal energy of a system increases when heat increases
The First Law of Thermodynamics, also known as the conservation of energy, states that energy cannot be created or destroyed but can be converted from one form to another. This law applies to all forms of energy, including heat, work, kinetic energy, and potential energy.
The internal energy of a system is the sum of all types of energy contained within it, including kinetic and potential energy. When heat is added to a system, it can increase, decrease, or leave the internal energy unchanged. This depends on the work done by the system on its surroundings.
The relationship between heat added to a system and the change in internal energy is described by the equation ΔU = Q - W, where ΔU represents the change in internal energy, Q is the heat added, and W is the work done by the system. If the heat added is greater than the work done (Q > W), the internal energy increases (ΔU > 0). If the heat added equals the work done (Q = W), the internal energy remains constant (ΔU = 0). If the work done is greater than the heat added (Q < W), the internal energy decreases (ΔU < 0).
For example, consider a gas in a cylinder. If the gas is compressed by pushing the piston down, the gas particles speed up and collide more frequently, increasing the internal energy of the system. This increase in internal energy is due to the added heat, which increases the kinetic energy of the gas particles.
The First Law of Thermodynamics helps us understand and quantify these energy exchanges and transformations within systems, providing a fundamental framework for the field of thermodynamics.
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The first law motivates the introduction of the concept of temperature
The first law of thermodynamics is a formulation of the law of conservation of energy in the context of thermodynamic processes. It states that the total energy of a system remains constant, even if it is converted from one form to another. This is because energy cannot be created or destroyed, only altered in form. The first law distinguishes two principal forms of energy transfer: heat and thermodynamic work.
The first law also defines the internal energy of a system, an extensive property that accounts for the balance of heat transfer, thermodynamic work, and matter transfer into and out of the system. The internal energy of a system is related to its temperature. If a system has a definite temperature, its total energy can be distinguished into kinetic energy, potential energy, and internal energy. Kinetic energy is the energy due to the motion of the system as a whole, while potential energy results from an externally imposed force field.
The first law of thermodynamics allows for many possible states of a system to exist. However, only certain states occur, and this leads to the second law of thermodynamics and the definition of another state variable called entropy. The first law, therefore, provides the foundation for the introduction and clarification of the concept of temperature.
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Frequently asked questions
The first law of thermodynamics is a formulation of the law of conservation of energy in the context of thermodynamic processes. It states that the amount of energy in a closed system remains constant and can be converted from one form to another, but it cannot be created or destroyed.
The first law of thermodynamics emerged from 17th and 18th-century scientists' efforts to understand the nature of heat. By the early 19th century, scientists understood that heat is a form of energy. The first explicit statement of the law was made by Rudolf Clausius in 1850.
The first law of thermodynamics defines the internal energy of a system, which is an extensive property that accounts for the balance of heat transfer, work, and matter transfer into and out of the system. The change in internal energy of a system is equal to the difference between the heat supplied to the system and the work done by the system.
The equation for the first law of thermodynamics is ΔU = Q - W, where ΔU is the change in internal energy, Q is the heat added to the system, and W is the work done by the system.
An example of the first law of thermodynamics is the conversion of kinetic energy to heat energy when a driver presses the brakes to slow down a car. Another example is the conversion of heat into mechanical work in a steam engine.










































