Thermodynamic Thermodynamic is the study which is concerned

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Thermodynamic

Thermodynamic

Thermodynamic • is the study which is concerned with the ways in which energy

Thermodynamic • is the study which is concerned with the ways in which energy stored in body and how energy transformation which involve heat and work take place. • It deals with the quantitative relationships of interconversion of the various forms of energy, including mechanical, chemical, electric, and radiant energy.

Thermodynamic properties include ØTemperature Øpressure Ømass Øvolume

Thermodynamic properties include ØTemperature Øpressure Ømass Øvolume

 An important application of thermodynamic is the biological system, most diets are based

An important application of thermodynamic is the biological system, most diets are based on simple energy balance (the net energy gained by a person is equal to the difference between the energy intake as food and energy expended by exercise)

Q/ what is heat and what is temperature ? Heat Temperature the form of

Q/ what is heat and what is temperature ? Heat Temperature the form of energy that is is a measure of hotness or transferred from one coldness , its considered place to another as a consequence of the as a thermodynamic temperature difference property , that is the between the two places measure of energy • Numerically it can be contained in amass expressed by (Joule) or (Calorie)

 • A thermodynamic system is simply defined as a quantity of matter or

• A thermodynamic system is simply defined as a quantity of matter or a region in space chosen for study • The region outside the system is called (surrounding) • The physical (or virtual) barriers that separate the system from its surrounding is called (Boundary)

types of systems that are used to describe thermodynamic properties: • 1/ open system

types of systems that are used to describe thermodynamic properties: • 1/ open system : can exchange both energy and matter with its surrounding • 2/ closed system : can exchange energy but not matter with its surrounding • 3/ isolated system : that cant exchange neither matter nor energy.

 • if two immiscible solvents, water and carbon tetrachloride, are confined in a

• if two immiscible solvents, water and carbon tetrachloride, are confined in a closed container and iodine is distributed between the two phases, each phase is an open system, yet the total system made up of the two phases is closed because it does not exchange matter with its surroundings.

Examples of thermodynamic systems

Examples of thermodynamic systems

kinds of processes that can be carried out in thermodynamic system

kinds of processes that can be carried out in thermodynamic system

Isothermal process are those processes in which the system is maintained at a constant

Isothermal process are those processes in which the system is maintained at a constant temperature An isothermal reaction may be carried out by placing the system in a large constanttemperature bath so that heat is drawn from or returned to it without affecting the temperature significantly. The isothermal system requires either open or closed system

Adiabatic process is the one in which no heat enter or leave the system

Adiabatic process is the one in which no heat enter or leave the system , this process require an isolated system and the temperature of the system may be changed A reaction carried on inside a sealed Dewar flask or “vacuum bottle” is adiabatic because the system is thermally insulated from its surroundings.

Spontaneous process is the one that occur naturally and take place with out intervention

Spontaneous process is the one that occur naturally and take place with out intervention ( ex. If a filled balloon is punctured , much of the contained gas is transferred to the atmosphere)

Thermodynamics is based on three “laws” or facts of experience that have never been

Thermodynamics is based on three “laws” or facts of experience that have never been proven in a direct way, in part due to the ideal conditions for which they were derived. Various conclusions, usually expressed in the form of mathematical equations, however, may be deduced from these three principles, and the results consistently agree with observations.

 • If two bodies are in thermal equilibrium with a third body ,

• If two bodies are in thermal equilibrium with a third body , they are in thermal equilibrium with each other , this simple fact is known as (Zeroth law) • Note : the work of thermometer depends upon this law

First Law of Thermodynamics.

First Law of Thermodynamics.

The first law is a statement of the conservation of energy. It states that,

The first law is a statement of the conservation of energy. It states that, although energy can be transformed from one kind into another, it cannot be created or destroyed. Put in another way, the total energy of a system and its immediate surroundings remains constant during any operation. This statement follows from the fact that the various forms of energy are equivalent, and when one kind is formed, an equal amount of another kind must disappear.

The relativistic picture of the universe expressed by Einstein's equation Energy = (mass change)

The relativistic picture of the universe expressed by Einstein's equation Energy = (mass change) * (velocity of light)² suggests that matter can be considered as another form of energy, 1 g being equivalent to 9 × 1013 joules. These enormous quantities of energy are involved in nuclear transformations but are not important in ordinary chemical reactions.

According to the first law, the effects of Q (heat absorbed ) and W

According to the first law, the effects of Q (heat absorbed ) and W (work) in a given system during a transformation from an initial thermodynamic state to a final thermodynamic state are related to an intrinsic property of the system called the internal energy, defined as ∆E =E 2 -E 1 = Q+W where E 2 is the internal energy of the system in its final state and E 1 is the internal energy of the system in its initial state. The change in internal energy ΔE is related to Q and W transferred between the system and its surroundings the equation also expresses the fact that work and heat are equivalent ways of changing the internal energy of the system.

Work of Expansion Against a Constant Pressure • Imagine a vapor confined in a

Work of Expansion Against a Constant Pressure • Imagine a vapor confined in a hypothetical cylinder fitted with a weightless, frictionless piston of area A. If a constant external pressure Pex is exerted on the piston, the total force is Pex × A because P = Force/Area. The vapor in the cylinder is now made to expand by increasing the temperature, and the piston moves a distance h. The work done against the opposing pressure in one single stage is W=- Pex x A x h Now A × h is the increase in volume, ΔV = V 2 - V 1, so that, at constant pressure, W=- p ∆V = - Pex (v 2 –v 1)

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Thank you for listening