top of page

Temperature

Assumption:

In this calculation we are going to assume air is an ideal gas. Hence the ideal gas equation is as follows: 

Screen Shot 2019-09-25 at 10.53.35 PM.pn

Where:

p = pressure

V = Volume

R = Universal gas constant

T = Temperature in Kelvin

Calculation:

As the rocket expels the water, an adiabatic expansion of air takes place. From the first law of thermodynamics it is evident that during an adiabatic expansion, Q = 0. Adiabatic processes can be represented on a Pressure-Volume diagram as shown below: 

adiabatic_expansion.png

The internal energy can thus be calculated by the equation below:

Screen Shot 2019-09-25 at 10.55.27 PM.pn
Screen Shot 2019-09-26 at 11.47.00 AM.pn

Since it is an adiabatic expansion, dQ = 0

Therefore we get:

Screen Shot 2019-09-26 at 12.52.57 AM.pn

It is also known that:

Screen Shot 2019-09-26 at 12.54.53 AM.pn
Screen Shot 2019-09-26 at 11.49.47 AM.pn

Substituting the above equations in dU = -dW, we get:

Screen Shot 2019-09-26 at 1.00.48 AM.png

This relation can be graphically represented, as is shown below:

Picture1.png
Screen Shot 2019-09-27 at 5.05.16 PM.png

The starting temperature in the graph has been determined to be 298K (25°C). It can be seen that the temperature drops as the Volume increases and the water is expelled out of the rocket. This is predominantly due to the adiabatic expansion of the air. As the air has more space to fill out while the water gets expelled, there is a greater Volume. Here we have modeled the temperature as a function of time, for a period of 0.5 seconds. 

bottom of page