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An ice cube with a mass of \(25 \mathrm{~g}\) at \(-18{ }^{\circ} \mathrm{C}\) (typical freezer temperature) is dropped into a cup that holds \(250 \mathrm{~mL}\) of hot water, initially at \(85^{\circ} \mathrm{C}\). What is the final temperature in the cup? The density of liquid water is \(1.00 \mathrm{~g} / \mathrm{mL}\); the specific heat capacity of ice is \(2.03 \mathrm{~J} / \mathrm{g}{ }^{\circ} \mathrm{C} ;\) the specific heat capacity of liquid water is \(4.184 \mathrm{~J} / \mathrm{g}-\mathrm{K} ;\) the enthalpy of fusion of water is \(6.01 \mathrm{~kJ} / \mathrm{mol}\).

Short Answer

Expert verified
The final temperature in the cup is approximately \(75.18 °C\).

Step by step solution

01

Calculate the energy to heat the ice from -18°C to 0°C

To calculate the energy required to heat the ice from -18°C to 0°C, we use the formula for energy transfer: \(q = mc\Delta T\) Where: \(q\) = energy transfer (J), \(m\) = mass of the ice (g), \(c\) = specific heat capacity of the ice (J/g°C), and \(\Delta T\) = change in temperature (°C). Here, \(m = 25 g\), \(c = 2.03 J/g°C\), and \(\Delta T = 0°C - (-18°C) = 18 °C\). Thus, the energy required to heat the ice to 0°C is: \(q_1 = (25 g)(2.03 J/g °C)(18 °C) = 913.5 J\)
02

Calculate the energy to melt the ice at 0°C

To calculate the energy required to melt the ice at 0°C, we use the enthalpy of fusion (\(Qf\)). Given that the enthalpy of fusion of water is \(6.01 kJ/mol\), we first need to determine the number of moles in the ice cube: Number of moles = \(\frac{mass}{molar\,mass}\) Since the molar mass of water is 18 g/mol, the number of moles in 25g of ice is: \(\frac{25 g}{18 g/mol} = 1.389 mol\) Now, we can find the energy required to melt the ice: \(q_2 = nQ_f = (1.389 mol)(6.01 kJ/mol) = 8.35 kJ = 8350 J\)
03

Set up the equation to solve for the final temperature

To solve for the final temperature, we equate the energy absorbed in heating the ice cube to the energy released by the hot water. The energy absorbed is the sum of energies (\(q_1\) and \(q_2\)) from steps 1 and 2. Let T be the final temperature, then the energy released by hot water is given by the formula: \(q_3 = m_{water}c_{water}\Delta T_{water}\) The mass of hot water can be determined from its volume and density: \(m_{water} = 250 \,mL * \frac{1.00\,g}{1\,mL} = 250\,g\) And, \(\Delta T_{water} = T_{initial} - T_{final} = 85 °C - T\) Hence, the energy loss by the hot water can be represented as: \(q_3 = (250 g)(4.184 J/g °C)(85 °C - T)\) Now we equate the energy absorbed in heating the ice cube (sum of \(q_1\) and \(q_2\)) to the energy released by the hot water (\(q_3\)): \(q_1 + q_2 = q_3\) \(913.5 J + 8350 J = (250 g)(4.184 J/g °C)(85 °C - T)\) Now, solving the equation for the final temperature, T: \((85 °C - T) = \frac{913.5 J + 8350 J}{(250 g)(4.184 J/g °C)}\) \((85 °C - T) ≈ 9.818 °C\) Upon finding the difference: \(T ≈ 85 °C - 9.818 °C ≈ 75.18 °C\) So, the final temperature in the cup is approximately \(75.18 °C\).

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Key Concepts

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

Specific Heat Capacity
Specific heat capacity is a fundamental concept in thermochemistry that describes how much energy is needed to change the temperature of a substance. For ice, the specific heat capacity is given as \(2.03 \; \text{J/g}^\circ\text{C}\), which means it takes 2.03 Joules of energy to raise the temperature of one gram of ice by one degree Celsius. This property is crucial when calculating energy changes in substances, such as heating the ice from \(-18^\circ\text{C} \) to \(0^\circ\text{C}\).
We use the formula \( q = mc\Delta T \) to determine the energy transfer involved:
  • \( q \): energy (Joules)
  • \( m \): mass (grams)
  • \( c \): specific heat capacity
  • \( \Delta T \): temperature change (\circC)
Understanding specific heat capacity is key as it helps predict how substances will behave under temperature changes. It varies between materials; for example, water in liquid form has a specific heat capacity of \(4.184\; \text{J/g-K}\), allowing it to absorb heat efficiently, influencing everyday phenomena and technological applications.
Enthalpy of Fusion
The enthalpy of fusion is the amount of energy needed to turn a solid into a liquid at its melting point without changing its temperature. For water, this value is \(6.01 \text{kJ/mol}\). This indicates that it requires 6.01 kJ of energy to melt one mole of ice at \(0^\circ \text{C}\) into water.
In the exercise, after the ice is warmed to \(0^\circ \text{C}\), the next step is calculating how much energy is required to convert it to liquid water. This is done using the equation:
  • \( q_f = nQ_f \)
Where:
  • \( q_f \): the energy needed to melt the ice (Joules)
  • \( n \): number of moles of the substance
  • \( Q_f \): enthalpy of fusion (kJ/mol)
This energy calculation plays a crucial role in determining phase changes, enabling one to understand thermal dynamics in natural and industrial processes. It's a significant part of energy transfer calculations in thermochemical reactions.
Energy Transfer
Energy transfer is a critical concept in thermochemistry. It describes how energy moves from one system or object to another. In our scenario, energy is transferred from hot water to ice.
When the ice cube is added to the hot water, it absorbs energy and raises its temperature while simultaneously transferring energy to the ice, causing it to melt. How energy transfers can be calculated using the principle of conservation of energy. The energy lost by the hot water should equal the total energy the ice cube absorbs as it warms up and melts.
The relevant formula is:
  • \( q_\text{absorbed} = q_\text{released} \)
  • \( q_\text{absorbed} = q_1 + q_2 \) (heating + melting)
  • \( q_\text{released} = m c \Delta T \) for the hot water
Breaking down energy transfer into these steps makes it easier to solve complex problems and gain insights into energy dynamics in various reactions and processes, becoming a valuable tool in fields like chemistry, physics, and engineering.

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Most popular questions from this chapter

The \(K_{b}\) for methylamine \(\left(\mathrm{CH}_{3} \mathrm{NH}_{2}\right)\) at \(25^{\circ} \mathrm{C}\) is given in Appendix \(D\). (a) Write the chemical equation for the equilibrium that corresponds to \(K_{b}\). (b) By using the value of \(K_{b}\), calculate \(\Delta G^{\circ}\) for the equilibrium in part (a). (c) What is the value of \(\Delta G\) at equilibrium? (d) What is the value of \(\Delta G\) when \(\left[\mathrm{H}^{+}\right]=6.7 \times 10^{-9} \mathrm{M},\left[\mathrm{CH}_{3} \mathrm{NH}_{3}^{+}\right]=2.4 \times 10^{-3} \mathrm{M}\) and \(\left[\mathrm{CH}_{3} \mathrm{NH}_{2}\right]=0.098 \mathrm{M} ?\)

A standard air conditioner involves a \(r\) frigerant that is typically now a fluorinated hydrocarbon, such as \(\mathrm{CH}_{2} \mathrm{~F}_{2}\). An air- conditioner refrigerant has the property that it readily vaporizes at atmospheric pressure and is easily compressed to its liquid phase under increased pressure. The operation of an air conditioner can be thought of as a closed system made up of the refrigerant going through the two stages shown here (the air circulation is not shown in this diagram). During expansion, the liquid refrigerant is released into an expansion chamber at low pressure, where it vaporizes. The vapor then undergoes compression at high pressure back to its liquid phase in a compression chamber. (a) What is the sign of \(q\) for the expansion? (b) What is the sign of \(q\) for the compression? (c) In a central air-conditioning system, one chamber is inside the home and the other is outside. Which chamber is where, and why? (d) Imagine that a sample of liquid refrigerant undergoes expansion followed by compression, so that it is back to its original state. Would you expect that to be a reversible process? (e) Suppose that a house and its exterior are both initially at \(31^{\circ} \mathrm{C}\). Some time after the air conditioner is turned on, the house is cooled to \(24^{\circ} \mathrm{C}\). Is this process spontaneous of nonspontaneous?

Indicate whether each statement is true or false. (a) \(\Delta S\) depends on whether the process is reversible or irreversible. \((\mathbf{b})\) If a system undergoes an irreversible change, the entropy of the universe increases. (c) Only if the change in entropy of the system is exactly matched by an equal and opposite change in the entropy of the surroundings, the system undergoes a reversible process. (d) If the entropy change of the system is zero, the system undergoes a reversible process.

Using \(S^{\circ}\) values from Appendix \(\mathrm{C}\), calculate \(\Delta S^{\circ}\) values for the following reactions. In each case, account for the sign of \(\Delta S\). (a) \(\mathrm{NH}_{4} \mathrm{Cl}(s) \longrightarrow \mathrm{NH}_{4}^{+}(a q)+\mathrm{Cl}^{-}(a q)\) (b) \(\mathrm{CH}_{3} \mathrm{OH}(g) \longrightarrow \mathrm{CO}(g)+2 \mathrm{H}_{2}(g)\) (c) \(\mathrm{CH}_{4}(g)+2 \mathrm{O}_{2}(g) \longrightarrow \mathrm{CO}_{2}(g)+2 \mathrm{H}_{2} \mathrm{O}(g)\) (d) \(\mathrm{CH}_{4}(g)+2 \mathrm{O}_{2}(g) \longrightarrow \mathrm{CO}_{2}(g)+2 \mathrm{H}_{2} \mathrm{O}(l)\)

When most elastomeric polymers (e.g., a rubber band) are stretched, the molecules become more ordered, as illustrated here: Suppose you stretch a rubber band. (a) Do you expect the entropy of the system to increase or decrease? (b) If the rubber band were stretched isothermally, would heat need to be absorbed or emitted to maintain constant temperature? (c) Try this experiment: Stretch a rubber band and wait a moment. Then place the stretched rubber band on your upper lip, and let it return suddenly to its unstretched state (remember to keep holding on!). What do you observe? Are your observations consistent with your answer to part (b)?

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