Welcome to this fascinating journey through thermodynamics! Today, we are going to dissect a beautiful problem involving a cyclic process of an ideal gas. At first glance, graphs can be deceiving, but by carefully analyzing the axes and the physical laws governing the gas, we can unravel the entire story. Let's dive in!
Decoding the V-T Graph
The very first step in tackling any graphical thermodynamics problem is to look at the axes. It is a common pitfall to assume every graph is a p−V (pressure-volume) diagram. Here, the vertical axis represents Volume (V) and the horizontal axis represents Temperature (T).
We are given one mole of an ideal gas undergoing a cyclic process ABCA. Let's trace its path. The process starts at state A, where the temperature is T0 and the volume is V0. The pressure at this initial state is given as p0.
The Isothermal Journey from A to B
Look closely at the line connecting state A to state B. It is a perfectly vertical line. On a V−T graph, a vertical line means that the temperature is not changing. Therefore, TA=TB=T0. A process where the temperature remains constant is called an isothermal process.
Now, what does this mean for the internal energy of the gas? The internal energy (U) of an ideal gas is a function of its absolute temperature alone, given by the relation U=2fnRT. Since the temperature at A and B is exactly the same, their internal energies must also be identical. This confirms that Internal energies at A and B are the same.
Next, let's calculate the work done during this isothermal expansion. The gas expands from an initial volume V0 to a final volume 4V0. The work done in an isothermal process is given by the elegant formula:
Substituting our known values (n=1, T=T0, Vi=V0, Vf=4V0), we get:
WAB=RT0ln(V04V0)=RT0ln4
We can express this in terms of the initial pressure and volume. Using the ideal gas equation at state A, we know that pAVA=nRTA, which translates to p0V0=RT0. Substituting this back into our work equation, we find:
This perfectly matches our second option!
The Ambiguity of Process BC
Now, let's move from state B to state C. The graph shows a straight line connecting these two points. Here is where many students fall into a trap. It is tempting to assume that this straight line represents an isobaric (constant pressure) process.
For a process to be isobaric on a V−T graph, the volume must be directly proportional to the temperature (V∝T), which means the straight line must pass through the origin.
If we assume the line BC passes through the origin, we could calculate the pressure at C. Since AB is isothermal, pAVA=pBVB, giving us pB=4p0. An isobaric process would mean pC=pB=4p0. Furthermore, using Charles's Law (V/T=constant), we would find TC=4T0.
However, the graph does not explicitly show or state that the line BC passes through the origin. In physics, we cannot make assumptions based on visual approximations unless explicitly stated. Because of this crucial missing piece of information, we cannot definitively determine the pressure and temperature at state C.
Thus, we must conclude that only the first two statements are verifiably correct. This problem is a brilliant reminder to always read graphs carefully and never assume information that isn't explicitly provided!