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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) Normal body temperature. The average normal body temperature measured in the mouth is \(310 \mathrm{~K}\). What would Celsius and Fahrenheit thermometers read for this temperature? (b) Elevated body temperature. During very vigorous exercise, the body's temperature can go as high as \(40^{\circ} \mathrm{C}\). What would Kelvin and Fahrenheit thermometers read for this temperature? (c) Temperature difference in the body. The surface temperature of the body is normally about \(7 \mathrm{C}^{\circ}\) lower than the internal temperature. Express this temperature difference in kelvins and in Fahrenheit degrees. (d) Blood storage. Blood stored at \(4.0^{\circ} \mathrm{C}\) lasts safely for about 3 weeks, whereas blood stored at \(-160^{\circ} \mathrm{C}\) lasts for 5 years. Express both temperatures on the Fahrenheit and Kelvin scales. (e) Heat stroke. If the body's temperature is above \(105^{\circ} \mathrm{F}\) for a prolonged period, heat stroke can result. Express this temperature on the Celsius and Kelvin scales.

A Styrofoam bucket of negligible mass contains \(1.75 \mathrm{~kg}\) of water and \(0.450 \mathrm{~kg}\) of ice. More ice, from a refrigerator at \(-15.0^{\circ} \mathrm{C},\) is added to the mixture in the bucket, and when thermal equilibrium has been reached, the total mass of ice in the bucket is \(0.884 \mathrm{~kg} .\) Assuming no heat exchange with the surroundings, what mass of ice was added?

One suggested treatment for a person who has suffered a stroke is immersion in an ice-water bath at \(0^{\circ} \mathrm{C}\) to lower the body temperature, which prevents damage to the brain. In one set of tests, patients were cooled until their internal temperature reached \(32.0^{\circ} \mathrm{C}\). To treat a \(70.0 \mathrm{~kg}\) patient, what is the minimum amount of ice (at \(0^{\circ} \mathrm{C}\) ) you need in the bath so that its temperature remains at \(0^{\circ} \mathrm{C} ?\) The specific heat of the human body is \(3480 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{C}^{\circ},\) and recall that normal body temperature is \(37.0^{\circ} \mathrm{C}\).

A industrious explorer of the polar regions has devised a contraption for melting ice. It consists of a sealed \(10 \mathrm{~L}\) cylindrical tank with a porous grate separating the top half from the bottom half. The bottom half includes a paddle wheel attached to an axle that passes outside the cylinder, where it is attached by a gearbox and pulley system to a stationary bicycle. Pedaling the bicycle rotates the paddle wheel inside the cylinder. The tank includes \(6.00 \mathrm{~L}\) of water and \(3.00 \mathrm{~kg}\) of ice at \(0.0^{\circ} \mathrm{C}\). The water fills the bottom chamber, where it may be agitated by the paddle wheel, and partially fills the upper chamber, which also includes the ice. The bicycle is pedaled with an average torque of \(25.0 \mathrm{~N} \cdot \mathrm{m}\) at a rate of 30.0 revolutions per minute. The system is \(70 \%\) efficient. (a) For what length of time must the explorer pedal the bicycle to melt all the ice? (b) How much longer must he pedal to raise the temperature of the water to \(10.5^{\circ} \mathrm{C}\) ?

Animals in cold climates often depend on \(t w o\) layers of insulation: a layer of body fat (of thermal conductivity \(0.20 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) ) surrounded by a layer of air trapped inside fur or down. We can model a black bear (Ursus americanus) as a sphere \(1.5 \mathrm{~m}\) in diameter having a layer of fat \(4.0 \mathrm{~cm}\) thick. (Actually, the thickness varies with the season, but we are interested in hibernation, when the fat layer is thickest.) In studies of bear hibernation, it was found that the outer surface layer of the fur is at \(2.7^{\circ} \mathrm{C}\) during hibernation, while the inner surface of the fat layer is at \(31.0^{\circ} \mathrm{C}\). (a) What is the temperature at the fat-inner fur boundary so that the bear loses heat at a rate of \(50.0 \mathrm{~W} ?\) (b) How thick should the air layer (contained within the fur) be?

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