A process by which a gas does work on a piston at constant pressure is called an
isobaric process
. Such processes are examples of a
thermodynamic process
.
A thermodynamic process describes a change that happens to a gas, which results in change in its pressure \( P \), volume \( V \), and/or temperature \(T\)
T
T
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. An
isobaric
process is a thermodynamic process that takes place under constant pressure (so the volume and temperature of the gas may change in an isobaric process).
There are three more named thermodynamic processes. These processes are given special names because, like the isobaric process, they occur under some restrictions, which gives them their special properties, as described briefly below. These three additional named thermodynamic processes are:
isochoric
,
isothermal
, and
adiabatic
processes.
An
isochoric process
is a thermodynamic process in which no change in volume takes place. Because the work done by a gas is proportional to the change in volume, in an isochoric process, no work is done by (or on) the gas. Instead, in an isochoric process, a heat transfer takes place, and the energy from the heat transfer goes into increasing (or decreasing) the internal energy of the gas, increasing (or decreasing) its temperature.
An
isothermal process
is a thermodynamic process in which no change in temperature takes place. A gas expanding isothermally, for example, does work on the surrounding, but its internal energy (as represented by the temperature) does not change, because enough heat flows in to balance out the energy expended in doing work. This is consistent with the first law of thermodynamics since \(Q=W\). An isothermal process occurs if a thermodynamic process in a gas occurs slowly enough so that the gas remains in thermal equilibrium with the surroundings at all times.
The adiabatic process is, in some sense, the opposite of an isothermal process. In an
adiabatic process
, no heat transfer takes place (that is \(Q=0\)). This may happen because the gas is well-insulated from the surroundings. It may also happen because the process occurs so quickly that no significant heat transfer can take place. In an adiabatic expansion, for example, the internal energy of the gas decreases, because of the work done by the gas in expansion. This is perhaps the clearest experimental evidence one can observe that it takes work for a gas to expand under pressure.
Both isothermal and adiabatic processes are reversible in principle. A
reversible process
is one in which both the system and its environment can return to exactly the states they were in by following the reverse path. The reverse isothermal and adiabatic paths are BA and CA, respectively. Real macroscopic processes are never exactly reversible. In the previous examples, our system is a gas (like that in Figure \(\PageIndex{4}\)), and its environment is the piston, cylinder, and the rest of the universe. If there are any energy-dissipating mechanisms, such as friction or turbulence, then heat transfer to the environment occurs for either direction of the piston. So, for example, if the path BA is followed and there is friction, then the gas will be returned to its original state but the environment will not—it will have been heated in both directions. Reversibility requires the direction of heat transfer to reverse for the reverse path. Since dissipative mechanisms cannot be completely eliminated, real processes cannot be reversible.
There must be reasons that real macroscopic processes cannot be reversible. We can imagine them going in reverse. For example, heat transfer occurs spontaneously from hot to cold and never spontaneously the reverse. Yet it would not violate the first law of thermodynamics for this to happen. In fact, all spontaneous processes, such as bubbles bursting, never go in reverse. There is a second thermodynamic law that forbids them from going in reverse. When we study this law, we will learn something about nature and also find that such a law limits the efficiency of heat engines. We will find that heat engines with the greatest possible theoretical efficiency would have to use reversible processes, and even they cannot convert all heat transfer into doing work. The table summarizes the simpler thermodynamic processes and their definitions.
|
Isobaric
|
Constant pressure
|
\(W = P\Delta V\)
|
|
Isochoric
|
Constant volume
|
\(W = 0\)
|
|
Isothermal
|
Constant temperature
|
\(Q = W\)
|
|
Adiabatic
|
No heat transfer
|
\(Q = 0\)
|
PHET EXPLORATIONS: STATES OF MATTER
Watch different types of molecules form a solid, liquid, or gas in teh States of Matter simuator. Add or remove heat and watch the phase change. Change the temperature or volume of a container and see a pressure-temperature diagram respond in real time. Relate the interaction potential to the forces between molecules.
Summary
-
One of the important implications of the first law of thermodynamics is that machines can be harnessed to do work that humans previously did by hand or by external energy supplies such as running water or the heat of the Sun. A machine that uses heat transfer to do work is known as a heat engine.
-
There are several simple processes, used by heat engines, that flow from the first law of thermodynamics. Among them are the isobaric, isochoric, isothermal and adiabatic processes.
-
These processes differ from one another based on how they affect pressure, volume, temperature, and heat transfer.
-
If the work done is performed on the outside environment, work \((W)\) will be a positive value. If the work done is done to the heat engine system, work \((W)\) will be a negative value.
-
Some thermodynamic processes, including isothermal and adiabatic processes, are reversible in theory; that is, both the thermodynamic system and the environment can be returned to their initial states. However, because of loss of energy owing to the second law of thermodynamics, complete reversibility does not work in practice.
Glossary
-
heat engine
-
a machine that uses heat transfer to do work
-
isobaric process
-
constant-pressure process in which a gas does work
-
isochoric process
-
a constant-volume process
-
isothermal process
-
a constant-temperature process
-
adiabatic process
-
a process in which no heat transfer takes place
-
reversible process
-
a process in which both the heat engine system and the external environment theoretically can be returned to their original states
Contributors and Attributions
-
Paul Peter Urone (Professor Emeritus at California State University, Sacramento) and Roger Hinrichs (State University of New York, College at Oswego) with Contributing Authors: Kim Dirks (University of Auckland) and Manjula Sharma (University of Sydney). This work is licensed by OpenStax University Physics under a
Creative Commons Attribution License (by 4.0)
.