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A carpenter builds an exterior house wall with a layer of wood 3.0 cm thick on the outside and a layer of Styrofoam insulation 2.2 cm thick on the inside wall surface. The wood has \(k\) = 0.080 W/m \(\cdot\) K, and the Styrofoam has \(k\) = 0.027 W /m \(\cdot\) K. The interior surface temperature is 19.0\(^\circ\)C, and the exterior surface temperature is -10.0\(^\circ\)C. (a) What is the temperature at the plane where the wood meets the Styrofoam? (b) What is the rate of heat flow per square meter through this wall?

Short Answer

Expert verified
The interface temperature is -0.88°C; heat flow rate is 24.37 W/m².

Step by step solution

01

Understanding the Heat Flow Equation

The temperature at the interface and the rate of heat flow can be determined using thermal conductivity and the concept of steady-state heat conduction. The formula \[ q = \frac{T_1 - T_2}{R} \] is used, where \( q \) is the heat flow, \( T_1 \) and \( T_2 \) are temperatures, and \( R \) is the thermal resistance sum.
02

Calculate Thermal Resistance for Wood and Styrofoam

Thermal resistance \( R \) is calculated using the formula \( R = \frac{d}{k} \), where \( d \) is thickness and \( k \) is thermal conductivity. For wood, \( R_{\text{wood}} = \frac{0.030}{0.080} = 0.375 \) m²K/W. For Styrofoam, \( R_{\text{styrofoam}} = \frac{0.022}{0.027} = 0.815 \) m²K/W.
03

Find Total Thermal Resistance

The total thermal resistance \( R \) is the sum of the resistances of the wood and Styrofoam: \[ R_{\text{total}} = R_{\text{wood}} + R_{\text{styrofoam}} = 0.375 + 0.815 = 1.190 \text{ m}^2\cdot\text{K/W}. \]
04

Determine Temperature at Interface Using Temperature Drop Proportion

The temperature drop across each layer is proportional to its resistance. Given temperatures: \( T_{\text{inside}} = 19.0^\circ\text{C} \) and \( T_{\text{outside}} = -10.0^\circ\text{C} \). The total temperature drop is 29.0°C. Temperature drop across Styrofoam: \[ \Delta T_{\text{styrofoam}} = \frac{R_{\text{styrofoam}}}{R_{\text{total}}} \times 29 = \frac{0.815}{1.190} \times 29 = 19.88^\circ\text{C}. \] Thus, the interface temperature is \[ T_{\text{interface}} = T_{\text{inside}} - \Delta T_{\text{styrofoam}} = 19.0 - 19.88 = -0.88^\circ\text{C}. \]
05

Calculate Rate of Heat Flow per Square Meter

Using the total thermal resistance, the heat flow rate per square meter can be calculated as:\[ q = \frac{T_{\text{inside}} - T_{\text{outside}}}{R_{\text{total}}} = \frac{19.0 - (-10.0)}{1.190} = \frac{29.0}{1.190} = 24.37 \text{ W/m}^2. \]

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Key Concepts

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

Thermal Resistance
Thermal resistance is a way to measure how well a material can resist the flow of heat. Think of it as the thermal version of electrical resistance. Just like wires can resist the flow of electricity, materials can resist the flow of heat.
To calculate the thermal resistance (\( R \)) of a material, we use the formula: \[ R = \frac{d}{k} \]where:
  • \( d \) is the thickness of the material
  • \( k \) is the thermal conductivity, which tells us how well a material conducts heat
In our exercise with the wall, we have two layers: wood and Styrofoam. Each has its resistance based on its thickness and thermal conductivity:
  • Wood: Thickness is 0.030 m, \( k = 0.080 \) W/m·K, so \( R_{\text{wood}} = 0.375 \) m²K/W
  • Styrofoam: Thickness is 0.022 m, \( k = 0.027 \) W/m·K, so \( R_{\text{styrofoam}} = 0.815 \) m²K/W
By adding these resistances together, we get the total resistance of the wall, which is \( R_{\text{total}} = 1.190 \) m²K/W. This value shows how much the wall as a whole resists heat flow.
Heat Flow Equation
The heat flow equation helps us find out how much heat is moving through a material. It's like a formula that connects temperatures and thermal resistance.
The equation is: \[ q = \frac{T_1 - T_2}{R} \]where:
  • \( q \) is the rate of heat flow (measured in watts per square meter, W/m²)
  • \( T_1 \) and \( T_2 \) are the temperatures on either side of the material, measured in degrees Celsius
  • \( R \) is the total thermal resistance of the materials
In the wall example, the inside temperature (\( T_{\text{inside}} \)) is 19.0°C, and the outside temperature (\( T_{\text{outside}} \)) is -10.0°C. We already calculated \( R_{\text{total}} = 1.190 \) m²K/W for the entire wall.
Using these numbers, we apply the formula to find the heat flow:\[ q = \frac{19.0 - (-10.0)}{1.190} = \frac{29.0}{1.190} = 24.37 \text{ W/m}^2 \]The answer, 24.37 W/m², tells us how much heat escapes through each square meter of the wall.
Steady-State Conduction
Steady-state conduction refers to a condition where the temperatures are constant over time. It is like when a system reaches equilibrium, and heat flows at a constant rate.
Imagine a situation where heat constantly flows through a wall, but the temperatures inside and outside remain stable. This steady condition means we can predict how heat behaves over time.
In our example problem, we used steady-state conduction assumptions. It helped us find the temperature at the interface between the wood and Styrofoam. By finding out how much the temperature drops across each material layer, based on its resistance, we can understand how heat spreads through the wall.
Let's break it down:
  • The total temperature drop between the inside and outside of the wall is 29.0°C.
  • The temperature drop across the Styrofoam alone is calculated using its resistance proportion:
  • \[ \Delta T_{\text{styrofoam}} = \frac{R_{\text{styrofoam}}}{R_{\text{total}}} \times 29 = \frac{0.815}{1.190} \times 29 = 19.88°C \]
  • Thus, the temperature at the interface, going from inside to outside, is \( T_{\text{interface}} = 19.0 - 19.88 = -0.88°C \)
Understanding steady-state conduction helps predict real-world heat behavior in insulation and construction.

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Most popular questions from this chapter

BIO While running, a 70-kg student generates thermal energy at a rate of 1200 W. For the runner to maintain a constant body temperature of 37\(^\circ\)C, this energy must be removed by perspiration or other mechanisms. If these mechanisms failed and the energy could not flow out of the student’s body, for what amount of time could a student run before irreversible body damage occurred? (Note: Protein structures in the body are irreversibly damaged if body temperature rises to 44\(^\circ\)C or higher. The specific heat of a typical human body is 3480 J / kg \(\cdot\) K, slightly less than that of water. The difference is due to the presence of protein, fat, and minerals, which have lower specific heats.)

You have probably seen people jogging in extremely hot weather. There are good reasons not to do this! When jogging strenuously, an average runner of mass 68 kg and surface area 1.85 m\(^2\) produces energy at a rate of up to 1300 W, 80% of which is converted to heat. The jogger radiates heat but actually absorbs more from the hot air than he radiates away. At such high levels of activity, the skin's temperature can be elevated to around 33\(^\circ\)C instead of the usual 30\(^\circ\)C. (Ignore conduction, which would bring even more heat into his body.) The only way for the body to get rid of this extra heat is by evaporating water (sweating). (a) How much heat per second is produced just by the act of jogging? (b) How much net heat per second does the runner gain just from radiation if the air temperature is 40.0\(^\circ\)C (104\(^\circ\)F)? (Remember: He radiates out, but the environment radiates back in.) (c) What is the total amount of excess heat this runner's body must get rid of per second? (d) How much water must his body evaporate every minute due to his activity? The heat of vaporization of water at body temperature is \(2.42 \times 10{^6} J/kg\). (e) How many 750-mL bottles of water must he drink after (or preferably before!) jogging for a half hour? Recall that a liter of water has a mass of 1.0 kg.

Two rods, one made of brass and the other made of copper, are joined end to end. The length of the brass section is 0.300 m and the length of the copper section is 0.800 m. Each segment has cross-sectional area 0.00500 m\(^2\). The free end of the brass segment is in boiling water and the free end of the copper segment is in an ice–water mixture, in both cases under normal atmospheric pressure. The sides of the rods are insulated so there is no heat loss to the surroundings. (a) What is the temperature of the point where the brass and copper segments are joined? (b) What mass of ice is melted in 5.00 min by the heat conducted by the composite rod?

The operating temperature of a tungsten filament in an incandescent light bulb is 2450 K, and its emissivity is 0.350. Find the surface area of the filament of a 150-W bulb if all the electrical energy consumed by the bulb is radiated by the filament as electromagnetic waves. (Only a fraction of the radiation appears as visible light.)

A machinist bores a hole of diameter 1.35 cm in a steel plate that is at 25.0\(^\circ\)C. What is the cross-sectional area of the hole (a) at 25.0\(^\circ\)C and (b) when the temperature of the plate is increased to 175\(^\circ\)C? Assume that the coefficient of linear expansion remains constant over this temperature range.

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