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Thermodynamics
Module: General and Organic Chemistry (AOC106DI)
26 Documents
Students shared 26 documents in this course
University: Coventry University
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Thermodynamics
The study of energy and its link to chemical processes is known as thermodynamics. To
tackle thermodynamics difficulties, we must first define a system and its surroundings. The
object that undergoes a thermodynamic transformation is referred to as the system. The
system's environs are any parts of the universe in direct contact with it.
1. Open systems exchange mass as well as heat and energy with their environment.
2. Heat and energy are exchanged in closed systems, but not mass.
3. Heat/energy or mass are not exchanged between isolated systems.
The Thermodynamics First Law
The average total mechanical energy (kinetic + potential) of the particles that make up the
system is called internal energy.
The transfer of energy from a warmer to a cooler body is known as heat.
Thermal energy is transferred through molecule collisions, which necessitates direct physical
contact. Through molecular collisions, higher energy molecules in one system transmit some
of their energy to lower energy molecules in the other system.
Convection is the transmission of thermal energy through fluid movement. Due to pressure
or density differences, warm fluid travels in the direction of cooler fluid.
Radiation is the transfer of heat energy by electromagnetic waves. Metal, for example, emits
visible electromagnetic waves when heated and flaming red.
This first law asserts that the system's and its environment's energy is always conserved. This
indicates that any change to a system must be equal to the system's heat flow plus the
labour done on it.
ΔU = Q + W
ΔU = Change in internal energy
Q = Quantity of heat supplied to the system by its surroundings
W = net work done by the system
- Work done on system = + W
- Work done by system = - W
- Heat added to system = + Q
- Heat given off by system = - Q
In a cycle-like operation, the second rule of thermodynamics reveals that heat cannot be
totally converted to work. The preferred path of a particular transformation can be
determined using this law — for example, we know that heat flows from a hot source to a
cool source.