The Hidden Assumption in Heating
When we first learn about calorimetry, we are often taught the simple formula dQ=mCdT. For everyday substances like water at room temperature, it is perfectly fine to assume that the specific heat capacity C is a constant. This assumption leads to a beautifully straight, linear graph when we plot temperature against time under a constant heating rate.
However, the universe behaves very differently near absolute zero. When dealing with substances like liquid oxygen at 50 K, quantum mechanics takes the wheel. According to Debye's theory, the specific heat capacity of solids and liquids at very low temperatures is highly dependent on the temperature itself. As the temperature rises, the specific heat capacity C also increases. This single fact completely changes the geometry of our heating curve.
The Mathematics of the Slope
Let's translate this physical reality into mathematics. We are given that the rate of heating is constant. Let's call this constant power P.
Substituting
dQ=mCdT into our power equation, we get:
P=mCdtdT
To understand the shape of the Temperature-Time (
T−t) graph, we need to isolate its slope,
dtdT:
dtdT=mCP
Look closely at this master equation. The power P is constant, and the mass m is constant. The only variable on the right side is the specific heat C, which sits squarely in the denominator.
Decoding the Graphs
As the liquid oxygen absorbs heat, its temperature T increases. As we established earlier, an increasing temperature causes the specific heat C to increase.
Because C is growing larger and it is in the denominator, the overall fraction mCP must grow smaller. Therefore, the slope dtdT is continuously decreasing.
Geometrically, a decreasing slope means that the curve is getting flatter as time goes on. This creates a concave downward shape.
Once the liquid oxygen reaches its boiling point (around 90 K), it undergoes a phase change. During this time, all the supplied heat goes into breaking intermolecular bonds rather than raising the temperature. This gives us a perfectly horizontal line on the graph.
After boiling, the oxygen becomes a gas and begins to heat up again. The specific heat of the gas also slightly increases (or remains roughly constant) as vibrational modes begin to activate, meaning the slope will again decrease or remain constant, maintaining the concave downward or straight trajectory.
The Final Verdict
When we evaluate the given options, we are looking for a graph that starts with a concave downward curve, flattens out into a horizontal line, and then continues with another concave downward (or straight) curve. Graph (c) is the only option that flawlessly captures this physical reality.