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Energy, like matter, is always conserved, which means that it cannot be created or destroyed, but it can be converted from one form to another. Internal energy is a thermodynamic attribute of a system that refers to the energy associated with the system’s molecules and comprises both kinetic and potential energy. Whenever a system undergoes a change as a result of the interaction of heat, work, and internal energy, it is followed by a series of energy transfers and conversions. However, there is no net change in total energy throughout these exchanges. Similarly, the fundamental law of thermodynamics confirms that heat is a type of energy. This means that thermodynamic processes are guided by the concept of energy conservation. The first law of thermodynamics is often known as the Law of Energy Conservation. First Law of ThermodynamicsA thermodynamic system in equilibrium has a state variable known as internal energy (E). The difference in internal energy between two systems is equal to the difference between heat transfer into the system and work done by the system. The energy of the universe remains constant, according to the first law of thermodynamics. It can be exchanged between the system and the environment, but it cannot be generated or destroyed. The law is primarily concerned with changes in energy states caused by work and heat transmission. It reimagines the concept of energy conservation.
The equation for the first law of thermodynamics is given as; ΔU = q + W where: ΔU is the change in the internal energy of the system, q is the algebraic sum of heat transfer between system and surroundings, W is the work interaction of the system with its surroundings.
Limitations of First Law of Thermodynamics
First law of Thermodynamics for a Closed SystemWork done in a closed system is the product of pressure applied and volume change caused by applied pressure. W = − P ΔV Where P is the constant external pressure on the system, and ΔV is the change in volume of the system. This is specifically called pressure-volume work. The internal energy of a system rises or falls in response to work contact that occurs across its limits. Internal energy increases when work is performed on the system and decreases when work is performed by the system. Any heat interaction that occurs in the system with its surroundings modifies the system’s internal energy. However, because energy is constant (as stated by the first law of thermodynamics), the total change in internal energy is always zero. If the system loses energy, it is absorbed by the environment. When energy is absorbed by a system, it means that the energy was released by the environment: ΔUsystem = −ΔUsurroundings Where ΔUsystem is the change in the total internal energy of the system, and ΔUsurroundings is the change in the total energy of the surrounding. Applications of First Law of Thermodynamics
dQ = dU + dW ⇒ dQ = dW
A small amount of expansion occurs, i.e., ΔV = 0 ⇒ dW = PΔV = 0 So, dQ = dU + dW ⇒ dU = mL Thus, internal energy increases during the melting process.
The heat engine is the most common practical application of the First Law. Thermal energy is converted into mechanical energy via heat engines and vice versa. The vast majority of heat engines are open systems. A heat engine’s basic idea makes use of the correlations between heat, volume, and pressure of a working fluid. This fluid is normally a gas, however, it may transition from gas to liquid and back to gas during a cycle in some instances. When a gas is heated, it expands; nevertheless, when the same gas is confined, its pressure rises. If the confinement chamber’s bottom wall is the top of a moving piston, this pressure exerts a force on the piston’s surface, causing it to travel downward. This movement can then be used to provide work equal to the total force applied to the top of the piston multiplied by the distance traveled by the piston. Refrigerators, air conditioners, and heat pumps Refrigerators and heat pumps are mechanical energy converters that convert mechanical energy to heat. The majority of these are classified as closed systems. When a gas is compressed, its temperature rises. This hot gas can then radiate heat into its surroundings. When the compressed gas is allowed to expand, its temperature drops below what it was before compression because some of its heat energy was removed during the hot cycle. After then, the cold gas can absorb heat energy from its surroundings. This is the operating principle of an air conditioner. Air conditioners do not generate cold; rather, they remove heat. A mechanical pump transports the working fluid outside, where it is compressed and heated. The heat is then transferred to the outside environment, typically via an air-cooled heat exchanger. Then it is delivered indoors to expand and cool before taking heat from the internal air via another heat exchanger. A heat pump is basically a reverse-cycle air conditioner. The compressed working fluid’s heat is used to warm the building. It is then moved outdoors, where it expands and cools, allowing it to absorb heat from the outside air, which is normally warmer than the chilly working fluid even in winter. Sample QuestionsQuestion 1: What is the enthalpy of formation of the most stable form of an element in its standard state? Answer:
Question 2: State Hess’s law. Answer:
Question 3: Define the first law of thermodynamics. Answer:
Question 4: Many thermodynamically feasible reactions do not occur under ordinary conditions. Why? Answer:
Question 5: Why is the first law of thermodynamics important to the environment? Answer:
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Reffered: https://www.geeksforgeeks.org
Class 11 |
Type: | Geek |
Category: | Coding |
Sub Category: | Tutorial |
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