For a class demonstration, your physics instructor pours \(1.00 \mathrm{~kg}\) of steam at \(100.0^{\circ} \mathrm{C}\) over \(4.00 \mathrm{~kg}\) of ice at \(0.00^{\circ} \mathrm{C}\) and allows the system to reach equilibrium. He is then going to measure the temperature of the system. While the system reaches equilibrium, you are given the latent heats of ice and steam and the specific heat of water: \(L_{\text {ice }}=3.33 \cdot 10^{5} \mathrm{~J} / \mathrm{kg}\), \(L_{\text {steam }}=2.26 \cdot 10^{6} \mathrm{~J} / \mathrm{kg}, c_{\text {water }}=4186 \mathrm{~J} /\left(\mathrm{kg}^{\circ} \mathrm{C}\right) .\) You are asked to calculate the final equilibrium temperature of the system. What value do you find?

Short Answer

Expert verified
Based on the given problem where steam at 100°C is poured over ice at 0°C, calculate the final equilibrium temperature of the system.

Step by step solution

01

Calculate the heat lost by steam

To find the heat lost by the steam, we first need to calculate the heat required to condense the steam into water. This can be done using the latent heat of steam: \(Q_1 = m_{steam} \cdot L_{steam}\) Now, plug in the values: \(Q_1 = 1.00 \mathrm{~kg} \cdot 2.26 \cdot 10^{6} \mathrm{~J} / \mathrm{kg} = 2.26 \cdot 10^{6} \mathrm{~J}\)
02

Calculate the heat gained by ice

To find the heat gained by the ice, we first need to calculate the heat required to melt the ice into water. This can be done using the latent heat of ice: \(Q_2 = m_{ice} \cdot L_{ice}\) Now, plug in the values: \(Q_2 = 4.00 \mathrm{~kg} \cdot 3.33 \cdot 10^{5} \mathrm{~J} / \mathrm{kg} = 1.33 \cdot 10^{6} \mathrm{~J}\)
03

Compare heat transfer values

Compare the values of \(Q_1\) and \(Q_2\): If \(Q_1 > Q_2\), then all ice melts and the final state is water only. In this case, we will then calculate the equilibrium temperature assuming all ice has melted. If \(Q_1 < Q_2\), then all steam condenses and the final state is a mixture of water and ice. In this case, the equilibrium temperature will be \(0^{\circ}C\). Here, \(Q_1 = 2.26 \cdot 10^{6} \mathrm{~J} > Q_2 = 1.33 \cdot 10^{6} \mathrm{~J}\), which means all the ice melts and we have only water in the final state.
04

Calculate the final equilibrium temperature

Since all ice has melted, we will now calculate the heat required to raise the temperature of the water formed from ice: \(Q_3 = m_{ice} \cdot c_{water} \cdot \Delta T_{ice}\) And calculate the heat required to lower the temperature of the water formed from steam: \(Q_4 = m_{steam} \cdot c_{water} \cdot \Delta T_{steam}\) We set both heat transfer values to be equal, as the heat lost by the steam-water must be gained by the ice-water: \(Q_3 = Q_4 \Rightarrow m_{ice} \cdot c_{water} \cdot \Delta T_{ice} = m_{steam} \cdot c_{water} \cdot \Delta T_{steam}\) The equilibrium temperature can then be calculated by solving for the temperature difference: \(\Delta T_{eq} = \frac{m_{steam} \cdot \Delta T_{steam}}{m_{ice}}\) We know the initial temperatures of steam and ice, so we can find the temperature differences: \(\Delta T_{steam} = 100^{\circ} \mathrm{C} - T_{eq}\) \(\Delta T_{ice} = T_{eq} - 0^{\circ} \mathrm{C}\) Substituting the initial temperature values and masses of steam and ice, we find the equilibrium temperature: \(T_{eq} = \frac{1.00 \mathrm{~kg}\cdot(100^{\circ} \mathrm{C} - T_{eq})}{4.00 \mathrm{~kg}}\) Solve for \(T_{eq}\): \(T_{eq} = \frac{100}{5} = 20 ^{\circ} \mathrm{C}\) The final equilibrium temperature of the system is \(20^{\circ} \mathrm{C}\).

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Most popular questions from this chapter

A thermos bottle fitted with a piston is filled with a gas. Since the thermos bottle is well insulated, no heat can enter or leave it. The piston is pushed in, compressing the gas. a) What happens to the pressure of the gas? Does it increase, decrease, or stay the same? b) What happens to the temperature of the gas? Does it increase, decrease, or stay the same? c) Do any other properties of the gas change?

Suppose \(0.010 \mathrm{~kg}\) of steam (at \(100.00^{\circ} \mathrm{C}\) ) is added to \(0.10 \mathrm{~kg}\) of water (initially at \(\left.19.0^{\circ} \mathrm{C}\right)\). The water is inside an aluminum cup of mass \(35 \mathrm{~g}\). The cup is inside a perfectly insulated calorimetry container that prevents heat flow with the outside environment. Find the final temperature of the water after equilibrium is reached.

A 2.0 -kg metal object with a temperature of \(90^{\circ} \mathrm{C}\) is submerged in \(1.0 \mathrm{~kg}\) of water at \(20^{\circ} \mathrm{C}\). The water-metal system reaches equilibrium at \(32^{\circ} \mathrm{C}\). What is the specific heat of the metal? a) \(0.840 \mathrm{~kJ} / \mathrm{kg} \mathrm{K}\) b) \(0.129 \mathrm{~kJ} / \mathrm{kg} \mathrm{K}\) c) \(0.512 \mathrm{~kJ} / \mathrm{kg} \mathrm{K}\) b) \(0.129 \mathrm{~kJ} / \mathrm{kg} \mathrm{K}\) d) \(0.433 \mathrm{~kJ} / \mathrm{kg} \mathrm{K}\)

The radiation emitted by a blackbody at temperature \(T\) has a frequency distribution given by the Planck spectrum: $$ \epsilon_{T}(f)=\frac{2 \pi h}{c^{2}}\left(\frac{f^{3}}{e^{h f / k_{\mathrm{B}} T}-1}\right) $$ where \(\epsilon_{T}(f)\) is the energy density of the radiation per unit increment of frequency, \(v\) (for example, in watts per square meter per hertz), \(h=6.626 \cdot 10^{-34} \mathrm{~J} \mathrm{~s}\) is Planck's constant, \(k_{\mathrm{B}}=1.38 \cdot 10^{-23} \mathrm{~m}^{2} \mathrm{~kg} \mathrm{~s}^{-2} \mathrm{~K}^{-1}\) is the Boltzmann constant, and \(c\) is the speed of light in vacuum. (We'll derive this distribution in Chapter 36 as a consequence of the quantum hypothesis of light, but here it can reveal something about radiation. Remarkably, the most accurately and precisely measured example of this energy distribution in nature is the cosmic microwave background radiation.) This distribution goes to zero in the limits \(f \rightarrow 0\) and \(f \rightarrow \infty\) with a single peak in between those limits. As the temperature is increased, the energy density at each frequency value increases, and the peak shifts to a higher frequency value. a) Find the frequency corresponding to the peak of the Planck spectrum, as a function of temperature. b) Evaluate the peak frequency at temperature \(T=6.00 \cdot 10^{3} \mathrm{~K}\), approximately the temperature of the photosphere (surface) of the Sun. c) Evaluate the peak frequency at temperature \(T=2.735 \mathrm{~K}\), the temperature of the cosmic background microwave radiation. d) Evaluate the peak frequency at temperature \(T=300 . \mathrm{K}\), which is approximately the surface temperature of Earth.

In one of your rigorous workout sessions, you lost \(150 \mathrm{~g}\) of water through evaporation. Assume that the amount of work done by your body was \(1.80 \cdot 10^{5} \mathrm{~J}\) and that the heat required to evaporate the water came from your body. a) Find the loss in internal energy of your body, assuming the latent heat of vaporization is \(2.42 \cdot 10^{6} \mathrm{~J} / \mathrm{kg}\). b) Determine the minimum number of food calories that must be consumed to replace the internal energy lost (1 food calorie \(=4186\) J).

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