/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 12 (II) \(A\) hot iron horseshoe \(... [FREE SOLUTION] | 91Ó°ÊÓ

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(II) \(A\) hot iron horseshoe \((\) mass \(=0.40 \mathrm{~kg}),\) just forged (Fig. \(19-28\) ), is dropped into \(1.05 \mathrm{~L}\) of water in a \(0.30-\mathrm{kg}\) iron pot initially at \(20.0^{\circ} \mathrm{C}\). If the final equilibrium temperature is \(25.0^{\circ} \mathrm{C}\), estimate the initial temperature of the hot horseshoe.

Short Answer

Expert verified
We are given: - Mass of the horseshoe, \( m_h = 0.40 \text{ kg} \)- Volume of water, \( V_w = 1.05 \text{ L} = 1.05 \times 10^{-3} \text{ m}^3\)- Mass of water, \( m_w = 1.05 \text{ kg} \) (since the density of water is \( 1000 \text{ kg/m}^3 \))- Mass of the pot, \( m_p = 0.30 \text{ kg} \)- Initial temperature of water and pot, \( T_i = 20.0^{\circ}\text{C} \)- Final equilibrium temperature, \( T_f = 25.0^{\circ}\text{C} \)

Step by step solution

01

Identify Known Variables

We are given: - Mass of the horseshoe, \( m_h = 0.40 \text{ kg} \)- Volume of water, \( V_w = 1.05 \text{ L} = 1.05 \times 10^{-3} \text{ m}^3\)- Mass of water, \( m_w = 1.05 \text{ kg} \) (since the density of water is \( 1000 \text{ kg/m}^3 \))- Mass of the pot, \( m_p = 0.30 \text{ kg} \)- Initial temperature of water and pot, \( T_i = 20.0^{\circ}\text{C} \)- Final equilibrium temperature, \( T_f = 25.0^{\circ}\text{C} \)

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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 tells how much heat energy is needed to change the temperature of a unit mass of a substance by 1°C. Each material has its own specific heat capacity, \( c \, (\text{J/kg}^\circ\text{C}) \). For example, water has a specific heat capacity of approximately 4186 J/kg°C, which means it requires 4186 Joules of energy to raise 1 kilogram of water by 1°C.
For our exercise, we know the specific heat capacity values of the materials involved:
  • Water: 4186 J/kg°C
  • Iron (both the horseshoe and the pot): about 450 J/kg°C
These values are crucial because they determine how each material will respond to heat transfer during the temperature change. Knowing the specific heat capacities, we can calculate how much heat energy is gained or lost by each substance.
Thermal Equilibrium
Thermal equilibrium refers to a state where all components in a system reach the same temperature. No net heat transfer occurs between the objects once equilibrium is achieved.
In our scenario, the horseshoe, the pot, and the water are involved in a heat exchange until they all reach a common temperature of 25°C, i.e., the thermal equilibrium temperature. Here’s how it progresses:
  • The hot horseshoe releases heat.
  • The pot and water absorb the heat until the temperature stabilizes at 25°C.
This concept is important as it enables us to use the principle of conservation of energy to equate the heat lost by the horseshoe to the heat gained by the pot and the water. Calculating these heat exchanges allows us to estimate the initial temperature of the horseshoe.
Heat Transfer
Heat transfer is the flow of thermal energy from a hotter object to a cooler one until thermal equilibrium is reached. It can occur through conduction, convection, or radiation. Here, we're primarily looking at conduction, as heat flows directly from the hot horseshoe to the cooler water and pot.
In this exercise, we calculate the energy transferred using the formula: \[ q = m \times c \times \Delta T \\] Where:
  • \( q \) is the heat energy (Joules)
  • \( m \) is the mass of the substance (kg)
  • \( c \) is the specific heat capacity (J/kg°C)
  • \( \Delta T \) is the change in temperature (°C)
Heat lost by the hotter object equals the heat gained by the cooler objects. The trick is to calculate each one's heat transfer using this formula. We assume the sum of heat gained by water and pot equals the heat lost by the horseshoe to find the unknown initial temperature of the horseshoe.

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Most popular questions from this chapter

(I) Show that if the molecules of a gas have \(n\) degrees of freedom, then theory predicts \(C_{V}=\frac{1}{2} n R \quad\) and \(C_{P}=\frac{1}{2}(n+2) R\)

(II) A 1.0-L volume of air initially at 3.5 atm of (absolute) pressure is allowed to expand isothermally until the pressure is \(1.0 \mathrm{~atm} .\) It is then compressed at constant pressure to its initial volume, and lastly is brought back to its original pressure by heating at constant volume. Draw the process on a \(P V\) diagram, including numbers and labels for the axes.

A house has well-insulated walls \(19.5 \mathrm{~cm}\) thick (assume conductivity of air) and area \(410 \mathrm{~m}^{2},\) a roof of wood \(5.5 \mathrm{~cm}\) thick and area \(280 \mathrm{~m}^{2}\), and uncovered windows \(0.65 \mathrm{~cm}\) thick and total area \(33 \mathrm{~m}^{2} .\) ( \(a\) ) Assuming that heat is lost only by conduction, calculate the rate at which heat must be supplied to this house to maintain its inside temperature at \(23^{\circ} \mathrm{C}\) if the outside temperature is \(-15^{\circ} \mathrm{C}\). \((b)\) If the house is initially at \(12^{\circ} \mathrm{C}\), estimate how much heat must be supplied to raise the temperature to \(23^{\circ} \mathrm{C}\) within 30 min. Assume that only the air needs to be heated and that its volume is \(750 \mathrm{~m}^{3}\). ( \(c\) ) If natural gas costs \(\$ 0.080\) per kilogram and its heat of combustion is \(5.4 \times 10^{7} \mathrm{~J} / \mathrm{kg},\) how much is the monthly cost to maintain the house as in part \((a)\) for \(24 \mathrm{~h}\) each day, assuming \(90 \%\) of the heat produced is used to heat the house? Take the specific heat of air to be \(0.24 \mathrm{kcal} / \mathrm{kg} \cdot \mathrm{C}^{\circ}\)

(III) In the process of taking a gas from state a to state \(\mathrm{c}\) along the curved path shown in Fig. \(19-32,85 \mathrm{~J}\) of heat leaves the system and \(55 \mathrm{~J}\) of work is done on the system. (a) Determine the change in internal energy, \(E_{\text {int, a }}-E_{\text {int, c }}\) (b) When the gas is taken along the path cda, the work done by the gas is \(W=38 \mathrm{~J}\). How much heat \(Q\) is added to the gas in the process cda? (c) If \(P_{\mathrm{a}}=2.2 P_{\mathrm{d}},\) how much work is done by the gas in the process abc? ( \(d\) ) What is \(Q\) for path abc? \((e)\) If \(E_{\text {int, a }}-E_{\text {int }, \mathrm{b}}=15 \mathrm{~J},\) what is \(Q\) for the process bc? Here is a summary of what is given: $$ \begin{aligned} Q_{\mathrm{a} \rightarrow \mathrm{c}} &=-85 \mathrm{~J} \\ W_{\mathrm{a}->\mathrm{c}} &=-55 \mathrm{~J} \\ W_{\mathrm{cda}} &=38 \mathrm{~J} \\ E_{\text {int, } \mathrm{a}}-E_{\text {int }, \mathrm{b}} &=15 \mathrm{~J} \\ P_{\mathrm{a}} &=2.2 P_{\mathrm{d}} . \end{aligned} $$

(II) (a) How much energy is required to bring a 1.0-L pot of water at \(20^{\circ} \mathrm{C}\) to \(100^{\circ} \mathrm{C} ?\) ( \(b\) ) For how long could this amount of energy run a 100 -W lightbulb?

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