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The molar heat capacity of a certain substance varies with temperature according to the empirical equation $$ C=29.5 \mathrm{~J} / \mathrm{mol} \cdot \mathrm{K}+\left(8.20 \times 10^{-3} \mathrm{~J} / \mathrm{mol} \cdot \mathrm{K}^{2}\right) T $$ How much heat is necessary to change the temperature of \(3.00 \mathrm{~mol}\) of this substance from \(27^{\circ} \mathrm{C}\) to \(227^{\circ} \mathrm{C} ?\) (Hint: Use Eq. (17.18) in the form \(d Q=n C d T\) and integrate. \()\)

Short Answer

Expert verified
The total heat necessary to change the temperature of the substance from \(27^{\circ} \mathrm{C}\) to \(227^{\circ}\mathrm{C}\) is obtained by substituting the values for \(T_{i}\), \(T_{f}\), and \(n\) into the equation from the last step.

Step by step solution

01

Understand the Given Formula

We are given the molar heat capacity (C) formula as \(C=29.5 \mathrm{~J} / \mathrm{mol} \cdot \mathrm{K}+\left(8.20 \times 10^{-3} \mathrm{~J} / \mathrm{mol} \cdot \mathrm{K}^{2}\right) T\). This formula will need to be integrated over the given temperature range.
02

Convert Temperatures to Kelvin

The temperature change is given in degrees Celsius, but the constants in the heat capacity equation are given in terms of Kelvin. Therefore, convert the temperatures from Celsius to Kelvin by adding 273.15 to each. This makes initial temperature \(T_{i} = 27^\circ C + 273.15 = 300.15 K\) and final temperature \(T_{f} = 227^\circ C + 273.15 = 500.15 K\).
03

Integrate the Molar Heat Capacity

We now integrate the formula of molar heat capacity over the temperature interval from \(T_{i}\) to \(T_{f}\) to get the heat transfer for one mole: \(\int_{T_{i}}^{T_{f}}C dT = \int_{T_{i}}^{T_{f}}(29.5 + 8.20 \times 10^{-3} T ) dT = [29.5 T + 4.10 \times 10^{-3} T^2]_{T_{i}}^{T_{f}}\)
04

Compute the Heat Transfer for One Mole

Substitute \(T_{f}\) and \(T_{i}\) into the equation derived in the previous step to compute the heat transfer for one mole: \(Q_{1 \text{ mol}} = [29.5 \times 500.15 + 4.10 \times 10^{-3} \times (500.15)^2] - [29.5 \times 300.15 + 4.10 \times 10^{-3} \times (300.15)^2]\)
05

Compute the Total Heat Transfer

Multiply the heat transfer for one mole by the 3 moles of the substance to get the total heat transferred: \(Q = n Q_{1 \text{ mol}} = 3.00 \text{ mol} \times Q_{1 \text{ mol}}\)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Molar Heat Capacity
Molar heat capacity is an important concept in thermodynamics. It refers to the amount of heat needed to change the temperature of one mole of a substance by one degree Kelvin. This is written in the formula as \( C \), and it often varies with temperature for different substances. This variation is due to the changes in energies associated with the molecular configurations or states at different temperatures.

In our example, the molar heat capacity is expressed as:
  • \( C = 29.5 \, \mathrm{J/mol \cdot K} + (8.20 \times 10^{-3} \, \mathrm{J/mol \cdot K^2}) \cdot T \)
This equation indicates that the molar heat capacity increases linearly with temperature \( T \). The first term is a constant, and the second term, containing \( T \), shows dependency on temperature. Understanding this variation is crucial for calculating the amount of heat needed for any thermodynamic process.
Temperature Conversion
Temperature conversion is often necessary when dealing with heat capacity problems, since equations in thermodynamics typically use Kelvin. This conversion is straightforward, but essential, as the scales are different. To convert a temperature from Celsius to Kelvin, you simply add 273.15 to the Celsius temperature.

For instance, in the original problem, temperatures change from 27°C to 227°C, which in Kelvin is:
  • Initial temperature: \( T_{i} = 27^{\circ} C + 273.15 = 300.15 \, K \)
  • Final temperature: \( T_{f} = 227^{\circ} C + 273.15 = 500.15 \, K \)
This conversion ensures all calculations align with the international standard for thermodynamics, providing accuracy when integrating formulas and determining heat changes.
Integration in Thermodynamics
Integration is a powerful mathematical tool in thermodynamics, especially when dealing with equations where variables change. In the case of our exercise, integration helps calculate the total heat transfer over a temperature range.
  • Start with the differential form \( dQ = nC dT \), where \( n \) is the number of moles.
  • Integrate this over the limits of initial and final temperatures \( T_{i} \) and \( T_{f} \).
For our given formula, \( C = 29.5 + 8.20 \times 10^{-3} T \), integration over \( T_{i} \) to \( T_{f} \) is performed as follows:
  • The integral becomes: \( \int_{T_{i}}^{T_{f}} (29.5 + 8.20 \times 10^{-3} T) \, dT = [29.5T + 4.10 \times 10^{-3} T^2]_{T_{i}}^{T_{f}} \)
This evaluation provides the heat transfer for one mole. Multiply by the number of moles, here 3, for the total heat required. Thus, integration simplifies how we account for varying factors like temperature over specific ranges, offering a precise solution.

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Most popular questions from this chapter

A carpenter builds a solid wood door with dimensions \(2.00 \mathrm{~m} \times 0.95 \mathrm{~m} \times 5.0 \mathrm{~cm} .\) Its thermal conductivity is \(k=0.120 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The air films on the inner and outer surfaces of the door have the same combined thermal resistance as an additional \(1.8 \mathrm{~cm}\) thickness of solid wood. The inside air temperature is \(20.0^{\circ} \mathrm{C},\) and the outside air temperature is \(-8.0^{\circ} \mathrm{C}\). (a) What is the rate of heat flow through the door? (b) By what factor is the heat flow increased if a window \(0.500 \mathrm{~m}\) on a side is inserted in the door? The glass is \(0.450 \mathrm{~cm}\) thick, and the glass has a thermal conductivity of \(0.80 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The air films on the two sides of the glass have a total thermal resistance that is the same as an additional \(12.0 \mathrm{~cm}\) of glass.

A carpenter builds an exterior house wall with a layer of wood \(3.0 \mathrm{~cm}\) thick on the outside and a layer of Styrofoam insulation \(2.2 \mathrm{~cm}\) thick on the inside wall surface. The wood has \(k=0.080 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K},\) and the Styrofoam has \(k=0.027 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K} .\) The interior surface temperature is \(19.0^{\circ} \mathrm{C},\) and the exterior surface temperature is \(-10.0^{\circ} \mathrm{C}\). (a) What is the temperature at the plane where the wood meets the Styrofoam? (b) What is the rate of heat flow per square meter through this wall?

A laboratory technician drops a \(0.0850 \mathrm{~kg}\) sample of unknown solid material, at \(100.0^{\circ} \mathrm{C}\), into a calorimeter. The calorimeter can, initially at \(19.0^{\circ} \mathrm{C},\) is made of \(0.150 \mathrm{~kg}\) of copper and contains \(0.200 \mathrm{~kg}\) of water. The final temperature of the calorimeter can and contents is \(26.1^{\circ} \mathrm{C}\). Compute the specific heat of the sample.

In very cold weather a significant mechanism for heat loss by the human body is energy expended in warming the air taken into the lungs with each breath. (a) On a cold winter day when the temperature is \(-20^{\circ} \mathrm{C},\) what amount of heat is needed to warm to body temperature \(\left(37^{\circ} \mathrm{C}\right)\) the \(0.50 \mathrm{~L}\) of air exchanged with each breath? Assume that the specific heat of air is \(1020 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\) and that \(1.0 \mathrm{~L}\) of air has mass \(1.3 \times 10^{-3} \mathrm{~kg} .\) (b) How much heat is lost per hour if the respiration rate is 20 breaths per minute?

You put a bottle of soft drink in a refrigerator and leave it until its temperature has dropped \(10.0 \mathrm{~K}\). What is its temperature change in (a) \(\mathrm{F}^{\circ}\) and \((\mathrm{b}) \mathrm{C}^{\circ} ?\)

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