Thermodynamics and First Law of Thermodynamics

Thermodynamics deals with the heat energy and its transformation to other formats of energy’s.It deals with different formats of heat energy is, conversion and its applications.

Coordinates of Thermodynamics of the fundamental physical quantities basing on which thermodynamics is steadied.Temperature, pressure, volume, internal energy and entropy are some of the coordinates of Thermodynamics.

Temperature is a measure of heat energy. Body with high heat energy will have more temperature than the body with a low heat energy.

Pressure is defined as the force acting per unit area.

Internal energy is the energy that the system poses inside. In the case of a gas internal energy is the sum of potential energy due to the position of the gas molecules, translational kinetic energy you to the motion of the gas molecules, vibrational kinetic energy due to the oscillation of particles and rotational kinetic energy to do the rotation of molecules.

Depending on the nature of the gas either all of these energies or some of the energies are going to contribute for the internal energy.

We cannot measure the absolute energy of a body or a system and we can only measure the change in it.

Internal energy cannot do any external work.



There are some fundamental laws of thermodynamics. Among them  zero'th  law thermodynamics is the first one.

Definition

If two bodies A and B are in thermal equilibrium with a third body C separately, then  A and B are also in thermal equilibrium.

Work done by a gas

Consider a cylinder having a fixed area of cross-section. Let a gas at a pressure P is available in the system where the three sides of the system are closed and the fourth side is a movable piston.

Because of the expansion of the gas heater place a certain force on the piston and most the piston in the forward direction by a small distance. Basing on the deformation of the work done we can calculate the value as shown below.



If the volume increases in this process then the work done is treated as positive and vice versa.

Work done by the system is treated as positive and the work done on the system is treated as negative. Work done by the system produces in the expansion in the system and vice versa.

If the pressure is variable we shall integrate the equation to get the work done.

First law thermodynamics

The heat energy is given to a system is equal to the sum of change in its internal energy and the external work done by it.

This is nothing but law of conservation of energy. Energy is neither created, nor destroyed and it just converts from one format to another format. Heat the heat energy supplied is converted into the format of increase in internal energy and the external work done.

While applying this la we shall apply certain sign convention.

Heat given to the system is treated as positive and heat given by the system is treated as negative.

Increase in internal energy is treated as positive and a decrease in internal energy is treated as negative.

Work done by the system is treated as positive and the work done on the system is treated as negative.

We are going to solve small problem basing on the concept of first law thermodynamics where we need to apply proper sign convention.


Problem and solution

In a thermodynamic process, the pressure of a fixed mass of a gas is changed. In this process gas releases 20 is also of heat energy and trade jolts of work is done on the gas. If initial internal energy of the system is 30 J  what is the final internal energy?

We can solve this problem basing on the first law thermodynamics. According to the law the total heat energy supplied is equal to the sum of change in internal energy and the external work done.

As the system releases the heat energy shall be treated as negative.

Change in internal energy has to be calculated.

As the work is done on the system it shall be treated as negative.


The above diagram consists of another problem also. That problem is also solved basing on the same concept.

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Doppler Effect and Its Applications

The apparent change in the frequency due to the relative motion of source and observer is called Doppler Effect. We can experience the change in the frequency only when there is a relative motion. The original frequency of the source is not actually changing. Due to the relative motion it is appearing like changing and that’s why it is called as apparent change in frequency.

We can derive the equation for the apparent frequency in different possible cases. When the observer is in the motion he will receive more number of the waves than when he is in the state of rest. It is simply because waves are not only crossing him and he is also crossing the waves.



When the observer is crossing the stationary source there will be difference in the frequencies. If the observer is approaching the apparent frequency increases and when the observer is receding the apparent frequency decreases. The difference between these frequencies can be heard like beats to the observer. We can calculate the number of the beats as shown below.



There will be apparent change in the frequency even when the observer is the state of rest and the source is moving towards the Observer. Here is the source is approaching the observer, its wavelength towards the observer decreases and hence frequency increases. We can derive the equation for the apparent frequency in this case as shown below.



When the observer is in the state of the rest and source is approaching him, apparent frequency increases. When the source is moving away from the stationary observer, apparent frequency decreases. The difference between these two frequencies can be heard like the beats to the observer. We can derive the equation for the number of the beats as shown below.



When a source is revolving around the stationary observer, he is not going to have any Doppler effect experience. It is simply because there is no relative motion between the source and observer. No component of the velocity of the source is acting towards the observer and hence we cannot find any change in the frequency.



If the source is moving in the circular path and observer is far away from the Centre of the circular path, he can hear apparent frequency with different possible frequencies. When the source is moving away from the observer, apparent frequency decreases and vice versa. We can write the equation is as shown below.



When a source is moving by making an angle  to the direction of the observer, still there will be apparent change in the frequency due to the component of the velocity of the source towards Observer. We can write the equation for it as shown below.



Problem and solution



Problem and solution



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