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A \(40-\mathrm{L}\) electrical radiator containing heating oil is placed in a \(50-\mathrm{m}^{3}\) room. Both the room and the oil in the radiator are initially at \(10^{\circ} \mathrm{C}\). The radiator with a rating of \(2.4 \mathrm{kW}\) is now turned on. At the same time, heat is lost from the room at an average rate of \(0.35 \mathrm{kJ} / \mathrm{s}\). After some time, the average temperature is measured to be \(20^{\circ} \mathrm{C}\) for the air in the room, and \(50^{\circ} \mathrm{C}\) for the oil in the radiator. Taking the density and the specific heat of the oil to be \(950 \mathrm{kg} / \mathrm{m}^{3}\) and \(2.2 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C},\) respectively, determine how long the heater is kept on. Assume the room is well-sealed so that there are no air leaks.

Short Answer

Expert verified
Answer: The heater was kept on for approximately 32 minutes.

Step by step solution

01

Determine the Energy Supplied by the Radiator to the Room

To find the energy supplied by the radiator, we need to multiply the power rating of the radiator by the time for which it is on. Let's denote the time as \(t\). The power rating of the radiator is given as \(2.4\,\mathrm{kW}\), which is equal to \(2400\,\mathrm{J/s}\). Therefore, the energy supplied by the radiator is \(E_\text{supplied}= 2400t\,\mathrm{J}\).
02

Determine the Energy Gained by the Oil in the Radiator

To find the energy gained by the oil inside the radiator, we'll use the equation \(E_\text{oil}=mc\Delta T\), where \(m\) is mass, \(c\) is specific heat capacity, and \(\Delta T\) is the change in temperature. The initial temperature of the oil is given as \(10\,^{\circ}\mathrm{C}\) and the final temperature is \(50\,^{\circ}\mathrm{C}\). Therefore, \(\Delta T = 50 - 10 = 40\,^{\circ}\mathrm{C}\). The mass of oil in the radiator can be found using the equation \(m=\rho V\), where \(\rho\) is the density of oil and \(V\) is the volume of oil in the radiator. The density \(\rho\) is given as \(950\,\mathrm{kg/m^3}\) and the volume \(V\) as \(40\,\mathrm{L}\), which equals \(0.04\,\mathrm{m^3}\). Hence, mass \(m = 950 \times 0.04 = 38\,\mathrm{kg}\). The specific heat capacity of the oil, \(c\), is given as \(2.2\,\mathrm{kJ/kg\cdot^{\circ}\mathrm{C}}\), which equals \(2200\,\mathrm{J/kg\cdot^{\circ}\mathrm{C}}\). Now we can find the energy gained by the oil in the radiator: \(E_\text{oil} = 38 \times 2200 \times 40 = 3344000\,\mathrm{J}\).
03

Determine the Energy Gained by the Air in the Room

Similarly to step 2, we'll use the equation \(E_\text{air}=mc\Delta T\) to find the energy gained by the air in the room. The initial temperature of the air is \(10\,^{\circ}\mathrm{C}\), and the final temperature is \(20\,^{\circ}\mathrm{C}\). Therefore, \(\Delta T = 20 - 10 = 10\,^{\circ}\mathrm{C}\). The mass of air in the room can be found using the equation \(m=\rho V\), where \(\rho\) is the density of air and \(V\) is the volume of the room. Assuming the density of air is approximately \(1.2\,\mathrm{kg/m^3}\) and given that the volume of the room is \(50\,\mathrm{m^3}\), we find the mass of the air in the room to be \(m = 1.2 \times 50 = 60\,\mathrm{kg}\). The specific heat capacity of air, \(c\), is approximately \(1000\,\mathrm{J/kg\cdot^{\circ}\mathrm{C}}\). Now we can find the energy gained by the air in the room: \(E_\text{air} = 60 \times 1000 \times 10 = 600000\,\mathrm{J}\).
04

Determine the Energy Lost From the Room

Given that heat is lost from the room at an average rate of \(0.35\,\mathrm{kJ/s}\), which is equal to \(350\,\mathrm{J/s}\), we can find the total energy lost from the room during the time \(t\) as \(E_\text{lost} = 350t\,\mathrm{J}\).
05

Set Up and Solve the Energy Conservation Equation

Now we apply the energy conservation principle. The energy supplied by the radiator must be equal to the energy gained by the oil in the radiator, the energy gained by the air in the room, and the energy lost from the room: \(E_\text{supplied} = E_\text{oil} + E_\text{air} + E_\text{lost}\). Substituting the expressions from steps 1-4, we get \(2400t = 3344000 + 600000 + 350t\). Simplifying the equation, we get \(2050t = 3944000\). Solving for \(t\), we find that \(t = \dfrac{3944000}{2050} = 1924\) seconds. Converting seconds to minutes, we obtain \(t \approx 32\) minutes. Therefore, the heater is kept on for approximately 32 minutes.

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Most popular questions from this chapter

A piston-cylinder device contains \(50 \mathrm{kg}\) of water at \(250 \mathrm{kPa}\) and \(25^{\circ} \mathrm{C}\). The cross-sectional area of the piston is \(0.1 \mathrm{m}^{2} .\) Heat is now transferred to the water, causing part of it to evaporate and expand. When the volume reaches \(0.2 \mathrm{m}^{3}\) the piston reaches a linear spring whose spring constant is \(100 \mathrm{kN} / \mathrm{m} .\) More heat is transferred to the water until the piston rises \(20 \mathrm{cm}\) more. Determine \((a)\) the final pressure and temperature and ( \(b\) ) the work done during this process. Also, show the process on a \(P\) -V diagram.

The specific heat of a material is given in a strange unit to be \(c=3.60 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{F}\). The specific heat of this material in the SI units of \(\mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\) is \((a) 2.00 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\) (b) \(3.20 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\) \((c) 3.60 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\) \((d) 4.80 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\) \((e) 6.48 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\)

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One ton \((1000 \mathrm{kg})\) of liquid water at \(50^{\circ} \mathrm{C}\) is brought into a well-insulated and well-sealed \(4-\mathrm{m} \times 5-\mathrm{m} \times 6-\mathrm{m}\) room initially at \(15^{\circ} \mathrm{C}\) and 95 kPa. Assuming constant specific heats for both air and water at room temperature, determine the final equilibrium temperature in the room.

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