How does heat transfer occur?<\/h1><\/div><\/div><\/div><\/i><\/i><\/span>Read more<\/span><\/a><\/h4><\/div>- Heat Transfer<\/a>
- The First Law of Thermodynamics<\/a><\/li>
- Heat Transfer Mechanisms<\/a><\/li>
- \nConduction\n<\/a><\/li>
- \nConvection\n<\/a><\/li>
- \nRadiation\n<\/a><\/li><\/ul><\/li>
- Summary<\/a><\/li><\/ul><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div>
Heat Transfer<\/h2><\/div>Everyone knows that a cold water bottle will warm up if we leave it in a hot environment, and if we put the cold water bottle in a refrigerator, the water will become colder. We also know that heat will transfer from areas with high temperature to areas with low temperature. This phenomenon is scientifically called “Heat Transfer”.<\/p>\n<\/div>
The First Law of Thermodynamics<\/h3><\/div>The first law of thermodynamics is known by the principle of “Conservation of energy,” which states that “energy cannot be created or destroyed, but only transformed into other forms of energy.”<\/p>\n
From this statement, we can write the equation as:<\/p>\n
(Ein<\/sub>) – (Eout<\/sub>) = (\u0394Esystem<\/sub>)<\/p>\n\n- Ein<\/sub> <\/span>= Energy input to the system<\/li>\n
- Eout <\/span><\/sub>= Energy output from the system<\/li>\n
- \u0394Esystem <\/sub>= Energy change in the system<\/li>\n<\/ul>\n<\/div>
![\"The](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/energy-transfer.png\" "\\"energy-transfer\\"")
<\/span> <\/div>Figure 1: Diagram explaining the conservation of energy law with energy input, energy output, and changes\n<\/p><\/div><\/div><\/div>
Energy Balance for Closed Systems<\/h4><\/div>Closed Systems refers to systems where mass does not change such as a soda can at 12\u00b0C placed at room temperature of 25\u00b0C. Over time, the soda can temperature increases to 20\u00b0C<\/span><\/p>\nFrom the example, the soda can has the same mass of water as initially set, but receives heat from the outside environment which has a higher temperature (25\u00b0C), causing the soda can temperature to rise to 20\u00b0C (the water becomes warmer).<\/p>\n
We can write the equation as:<\/p>\n
(Ein<\/sub>) – (Eout<\/sub>) = (\u0394Esystem<\/sub>)<\/p>\n\u0394U = mcv<\/sub>\u0394T<\/p>\nor<\/p>\n
Q = mcv<\/sub>\u0394T<\/p>\n\n- \u0394U = <\/span>Energy change in the system, or \u0394Esystem<\/sub><\/li>\n
- Q = <\/span>Heat energy (kJ)<\/li>\n
- m = <\/span>Mass of the system (kg)<\/li>\n
- cv <\/sub>= <\/span>Specific heat capacity (kJ\/kg.K) <\/span><\/sub><\/li>\n
- \u0394T = <\/span>Temperature change (K)<\/li>\n<\/ul>\n<\/div>
![\"Energy](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/amount-of-energy-to-boil-water.png\" "\\"amount-of-energy-to-boil-water\\"")
<\/span> <\/div>Figure 2: Example image of a can and calculations\n<\/p><\/div><\/div><\/div>
Energy Balance for Open Systems (Steady-Flow System)<\/h4><\/div>Steady-Flow System is a system with constant flow where the mass flowing in equals the mass flowing out, such as a water pipe with water flowing inside, where the water flowing in at the beginning of the pipe equals the water flowing out at the end of the pipe. This system is called a Steady-Flow System.<\/p>\n
We can write the equation as:<\/p>\n
Q\u0307 = \u1e41cv<\/sub>\u0394T<\/p>\n\n- \u0394U = <\/span>Energy change in the system, or \u0394Esystem<\/sub><\/li>\n
- Q\u0307 = <\/span>Heat transfer rate (kJ\/s)<\/li>\n
- \u1e41 = <\/span>Mass flow rate (kg\/s)<\/li>\n
- cv <\/sub>= <\/span>Specific heat capacity (kJ\/kg.K) <\/span><\/sub><\/li>\n
- \u0394T = <\/span>Temperature change (K)<\/li>\n<\/ul>\n<\/div>
![\"steady](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/steady-Flow-System.png\" "\\"steady-Flow-System\\"")
<\/span> <\/div>Figure 3: Example image of flow inside a pipe<\/p><\/div><\/div><\/div><\/div><\/div><\/div><\/div>
Heat Transfer Mechanisms<\/h3><\/div>Heat transfer from one area to another can be accomplished in 3 ways:<\/p>\n
\n- Conduction<\/li>\n
- Convection<\/li>\n
- Radiation<\/li>\n<\/ol>\n<\/div>
\n- Conduction<\/li>\n<\/ul><\/h3><\/div>
Heat transfer that requires a medium including solids, liquids, and gases, where the medium is stationary with a fixed shape.<\/p>\n
For example:<\/p>\n
\n- Using metal chopsticks to pick up pork from a pan and feeling heat in your hand, because the metal chopsticks receive heat and transfer the heat to our hand.<\/li>\n
- Static air between building glass is also considered conduction.<\/li>\n<\/ul>\n<\/div>
![\"Heat](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/heat-conduction-in-chopstick.png\" "\\"heat-conduction-in-chopstick\\"")
<\/span> <\/div>Figure 4: Example image explaining heat conduction with chopsticks and fire<\/p><\/div><\/div><\/div>
Thermal Conductivity or K-Value<\/h4><\/div>As we know, when eating hot pot, we should use wooden chopsticks instead of metal chopsticks because wooden chopsticks won’t get hot, while metal chopsticks will get hot. Do we know why?<\/p>\n
What makes these two types of chopsticks different is the thermal conductivity (K-Value), which indicates how much heat can be transferred to the other side, depending on the type of material.<\/p>\n
\n- If the thermal conductivity coefficient is high, it means it can transfer a lot of heat.<\/li>\n
- If the thermal conductivity coefficient is low, it means it can transfer little heat.<\/li>\n<\/ul>\n<\/div>
![\"k-value\"](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/K-conductivity.png\" "\\"K-conductivity\\"")
<\/span> <\/div>Figure 5: Image showing the difference between materials with high and low thermal conductivity<\/p><\/div><\/div><\/div>
From the example, we can say that “metal” chopsticks have high thermal conductivity, while “wooden” chopsticks have low thermal conductivity.<\/p>\n
We can calculate the conduction heat transfer rate from:<\/p>\n
Q\u0307cond<\/sub> = kcond<\/sub> x A x (T1<\/sub> -T2<\/sub>) \/\u0394x<\/p>\n\n- Q\u0307cond <\/sub>= Conduction heat transfer rate (kJ\/s)<\/li>\n
- kcond <\/sub>= Thermal conductivity coefficient<\/li>\n
- A = Heat transfer area (m2<\/sup>)<\/li>\n
- T1 <\/sub>= Temperature at point 1 (K)<\/li>\n
- T2 <\/sub>= Temperature at point 2 (K)<\/li>\n
- \u0394x = Thickness of the medium (m)<\/li>\n<\/ul>\n<\/div>
![\"Heat](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/cal-heat-conduct.png\" "\\"cal-heat-conduct\\"")
<\/span> <\/div>Figure 6: Calculation example with accompanying illustration<\/p><\/div><\/div><\/div>
From this example, we can see that the lower the thermal conductivity coefficient, the lower the temperature on the other side. Therefore, we have another variable called “Thermal Resistance (R-Value)”.<\/p>\n<\/div>
Thermal Resistance or R-Value<\/h4><\/div>A variable that is opposite to the thermal conductivity coefficient (K-Value).<\/span><\/p>\n\n- If thermal resistance is high, it means the medium allows little heat to pass through.<\/li>\n
- If thermal resistance is low, it means the medium allows a lot of heat to pass through.<\/li>\n<\/ul>\n<\/div>
\n- Convection<\/li>\n<\/ul><\/h3><\/div>
The convection process is a process that relies on moving mediums, including liquids and gases, where the high-temperature part rises to the top and the low-temperature part sinks to the bottom, as we often hear “hot air rises, cold air sinks”.<\/p>\n
For example:<\/p>\n
\n- Tea boiling in a glass, where we can see tea leaves swirling vertically.<\/li>\n
- Air from an air compressor, which is quite hot.<\/li>\n<\/ul>\n<\/div>
![\"Heat](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/heat-convection-in-kettle.png\" "\\"heat-convection-in-kettle\\"")
<\/span> <\/div>Image of heat convection in a tea cup<\/p><\/div><\/div><\/div>
Convection depends on the characteristics of heat convection. For cold air, we can classify it as:<\/p>\n
\n- Free Convection (Natural Convection)<\/li>\n
- Forced Convection<\/li>\n<\/ol>\n
For example, on a very hot day after exercising, if we stay still, we call it “Free Convection,” but if we say it’s too hot and need to turn on a fan, we call it “Forced Convection”.<\/p>\n<\/div>
![\"Natural](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/forcenatural-convection.png\" "\\"force&natural-convection\\"")
<\/span> <\/div>Figure 7: Image of Free Convection and Forced Convection<\/p><\/div><\/div><\/div>
Convection Coefficient<\/h4><\/div>This variable tells us how much heat the environment at that moment can convect away.<\/p>\n
\n- If the convection coefficient is high, it means the fluid can carry away a lot of heat.<\/li>\n
- If the convection coefficient is low, it means the fluid can carry away little heat.<\/li>\n<\/ul>\n<\/div>
![\"Heat](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/Air-Water-Cool.png\" "\\"Air-&-Water-Cool\\"")
<\/span> <\/div>Figure 8: Image of fluids that can carry away different amounts of heat<\/p><\/div><\/div><\/div>
We can calculate the heat transfer rate from convection using Newton’s law of cooling:<\/p>\n
Q\u0307conv<\/sub> = hconv <\/sub>As <\/sub>(Ts<\/sub> -T\u221e<\/sub>)<\/p>\n\n- Q\u0307conv <\/sub>= Convection heat transfer rate (kJ\/s)<\/li>\n
- h<\/span>conv <\/sub>= Convection coefficient<\/li>\n
- As<\/sub> = Surface area where convection occurs (m2<\/sup>)<\/li>\n
- Ts <\/sub>= Object surface temperature (K)<\/li>\n
- T\u221e <\/sub>= Fluid temperature (K)<\/li>\n<\/ul>\n<\/div>
![\"Heat](\"https:\/\/3t-insulation.com\/wp-content\/uploads\/2020\/07\/cal-heat-convection.png\" "\\"cal-heat-convection\\"")
<\/span> <\/div>Figure 9: Image of heat convection calculation<\/p><\/div><\/div><\/div>
From this example, we can say that the amount of heat through convection depends on the values of:<\/p>\n
\n- h<\/span>conv <\/sub>Convection coefficient<\/li>\n
- As <\/sub>Surface area<\/li>\n
- T\u221e <\/sub>Fluid temperature<\/li>\n<\/ol>\n<\/div>
\n- Radiation<\/li>\n<\/ul><\/h3><\/div>
<\/i><\/i><\/span>Read more<\/span><\/a><\/h4><\/div>- Heat Transfer<\/a>
- The First Law of Thermodynamics<\/a><\/li>
- Heat Transfer Mechanisms<\/a><\/li>
- \nConduction\n<\/a><\/li>
- \nConvection\n<\/a><\/li>
- \nRadiation\n<\/a><\/li><\/ul><\/li>
- Summary<\/a><\/li><\/ul><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div>
Heat Transfer<\/h2><\/div>Everyone knows that a cold water bottle will warm up if we leave it in a hot environment, and if we put the cold water bottle in a refrigerator, the water will become colder. We also know that heat will transfer from areas with high temperature to areas with low temperature. This phenomenon is scientifically called “Heat Transfer”.<\/p>\n<\/div>
The First Law of Thermodynamics<\/h3><\/div>The first law of thermodynamics is known by the principle of “Conservation of energy,” which states that “energy cannot be created or destroyed, but only transformed into other forms of energy.”<\/p>\n
From this statement, we can write the equation as:<\/p>\n
(Ein<\/sub>) – (Eout<\/sub>) = (\u0394Esystem<\/sub>)<\/p>\n\n- Ein<\/sub> <\/span>= Energy input to the system<\/li>\n
- Eout <\/span><\/sub>= Energy output from the system<\/li>\n
- \u0394Esystem <\/sub>= Energy change in the system<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 1: Diagram explaining the conservation of energy law with energy input, energy output, and changes\n<\/p><\/div><\/div><\/div>
Energy Balance for Closed Systems<\/h4><\/div>Closed Systems refers to systems where mass does not change such as a soda can at 12\u00b0C placed at room temperature of 25\u00b0C. Over time, the soda can temperature increases to 20\u00b0C<\/span><\/p>\nFrom the example, the soda can has the same mass of water as initially set, but receives heat from the outside environment which has a higher temperature (25\u00b0C), causing the soda can temperature to rise to 20\u00b0C (the water becomes warmer).<\/p>\n
We can write the equation as:<\/p>\n
(Ein<\/sub>) – (Eout<\/sub>) = (\u0394Esystem<\/sub>)<\/p>\n\u0394U = mcv<\/sub>\u0394T<\/p>\nor<\/p>\n
Q = mcv<\/sub>\u0394T<\/p>\n\n- \u0394U = <\/span>Energy change in the system, or \u0394Esystem<\/sub><\/li>\n
- Q = <\/span>Heat energy (kJ)<\/li>\n
- m = <\/span>Mass of the system (kg)<\/li>\n
- cv <\/sub>= <\/span>Specific heat capacity (kJ\/kg.K) <\/span><\/sub><\/li>\n
- \u0394T = <\/span>Temperature change (K)<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 2: Example image of a can and calculations\n<\/p><\/div><\/div><\/div>
Energy Balance for Open Systems (Steady-Flow System)<\/h4><\/div>Steady-Flow System is a system with constant flow where the mass flowing in equals the mass flowing out, such as a water pipe with water flowing inside, where the water flowing in at the beginning of the pipe equals the water flowing out at the end of the pipe. This system is called a Steady-Flow System.<\/p>\n
We can write the equation as:<\/p>\n
Q\u0307 = \u1e41cv<\/sub>\u0394T<\/p>\n\n- \u0394U = <\/span>Energy change in the system, or \u0394Esystem<\/sub><\/li>\n
- Q\u0307 = <\/span>Heat transfer rate (kJ\/s)<\/li>\n
- \u1e41 = <\/span>Mass flow rate (kg\/s)<\/li>\n
- cv <\/sub>= <\/span>Specific heat capacity (kJ\/kg.K) <\/span><\/sub><\/li>\n
- \u0394T = <\/span>Temperature change (K)<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 3: Example image of flow inside a pipe<\/p><\/div><\/div><\/div><\/div><\/div><\/div><\/div>
Heat Transfer Mechanisms<\/h3><\/div>Heat transfer from one area to another can be accomplished in 3 ways:<\/p>\n
\n- Conduction<\/li>\n
- Convection<\/li>\n
- Radiation<\/li>\n<\/ol>\n<\/div>
\n- Conduction<\/li>\n<\/ul><\/h3><\/div>
Heat transfer that requires a medium including solids, liquids, and gases, where the medium is stationary with a fixed shape.<\/p>\n
For example:<\/p>\n
\n- Using metal chopsticks to pick up pork from a pan and feeling heat in your hand, because the metal chopsticks receive heat and transfer the heat to our hand.<\/li>\n
- Static air between building glass is also considered conduction.<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 4: Example image explaining heat conduction with chopsticks and fire<\/p><\/div><\/div><\/div>
Thermal Conductivity or K-Value<\/h4><\/div>As we know, when eating hot pot, we should use wooden chopsticks instead of metal chopsticks because wooden chopsticks won’t get hot, while metal chopsticks will get hot. Do we know why?<\/p>\n
What makes these two types of chopsticks different is the thermal conductivity (K-Value), which indicates how much heat can be transferred to the other side, depending on the type of material.<\/p>\n
\n- If the thermal conductivity coefficient is high, it means it can transfer a lot of heat.<\/li>\n
- If the thermal conductivity coefficient is low, it means it can transfer little heat.<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 5: Image showing the difference between materials with high and low thermal conductivity<\/p><\/div><\/div><\/div>
From the example, we can say that “metal” chopsticks have high thermal conductivity, while “wooden” chopsticks have low thermal conductivity.<\/p>\n
We can calculate the conduction heat transfer rate from:<\/p>\n
Q\u0307cond<\/sub> = kcond<\/sub> x A x (T1<\/sub> -T2<\/sub>) \/\u0394x<\/p>\n\n- Q\u0307cond <\/sub>= Conduction heat transfer rate (kJ\/s)<\/li>\n
- kcond <\/sub>= Thermal conductivity coefficient<\/li>\n
- A = Heat transfer area (m2<\/sup>)<\/li>\n
- T1 <\/sub>= Temperature at point 1 (K)<\/li>\n
- T2 <\/sub>= Temperature at point 2 (K)<\/li>\n
- \u0394x = Thickness of the medium (m)<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 6: Calculation example with accompanying illustration<\/p><\/div><\/div><\/div>
From this example, we can see that the lower the thermal conductivity coefficient, the lower the temperature on the other side. Therefore, we have another variable called “Thermal Resistance (R-Value)”.<\/p>\n<\/div>
Thermal Resistance or R-Value<\/h4><\/div>A variable that is opposite to the thermal conductivity coefficient (K-Value).<\/span><\/p>\n\n- If thermal resistance is high, it means the medium allows little heat to pass through.<\/li>\n
- If thermal resistance is low, it means the medium allows a lot of heat to pass through.<\/li>\n<\/ul>\n<\/div>
\n- Convection<\/li>\n<\/ul><\/h3><\/div>
The convection process is a process that relies on moving mediums, including liquids and gases, where the high-temperature part rises to the top and the low-temperature part sinks to the bottom, as we often hear “hot air rises, cold air sinks”.<\/p>\n
For example:<\/p>\n
\n- Tea boiling in a glass, where we can see tea leaves swirling vertically.<\/li>\n
- Air from an air compressor, which is quite hot.<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Image of heat convection in a tea cup<\/p><\/div><\/div><\/div>
Convection depends on the characteristics of heat convection. For cold air, we can classify it as:<\/p>\n
\n- Free Convection (Natural Convection)<\/li>\n
- Forced Convection<\/li>\n<\/ol>\n
For example, on a very hot day after exercising, if we stay still, we call it “Free Convection,” but if we say it’s too hot and need to turn on a fan, we call it “Forced Convection”.<\/p>\n<\/div>
<\/span> <\/div>Figure 7: Image of Free Convection and Forced Convection<\/p><\/div><\/div><\/div>
Convection Coefficient<\/h4><\/div>This variable tells us how much heat the environment at that moment can convect away.<\/p>\n
\n- If the convection coefficient is high, it means the fluid can carry away a lot of heat.<\/li>\n
- If the convection coefficient is low, it means the fluid can carry away little heat.<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 8: Image of fluids that can carry away different amounts of heat<\/p><\/div><\/div><\/div>
We can calculate the heat transfer rate from convection using Newton’s law of cooling:<\/p>\n
Q\u0307conv<\/sub> = hconv <\/sub>As <\/sub>(Ts<\/sub> -T\u221e<\/sub>)<\/p>\n\n- Q\u0307conv <\/sub>= Convection heat transfer rate (kJ\/s)<\/li>\n
- h<\/span>conv <\/sub>= Convection coefficient<\/li>\n
- As<\/sub> = Surface area where convection occurs (m2<\/sup>)<\/li>\n
- Ts <\/sub>= Object surface temperature (K)<\/li>\n
- T\u221e <\/sub>= Fluid temperature (K)<\/li>\n<\/ul>\n<\/div><\/span> <\/div>
Figure 9: Image of heat convection calculation<\/p><\/div><\/div><\/div>
From this example, we can say that the amount of heat through convection depends on the values of:<\/p>\n
\n- h<\/span>conv <\/sub>Convection coefficient<\/li>\n
- As <\/sub>Surface area<\/li>\n
- T\u221e <\/sub>Fluid temperature<\/li>\n<\/ol>\n<\/div>
\n- Radiation<\/li>\n<\/ul><\/h3><\/div>
- Heat Transfer<\/a>
- The First Law of Thermodynamics<\/a><\/li>
- Heat Transfer Mechanisms<\/a><\/li>
- \nConduction\n<\/a><\/li>
- \nConvection\n<\/a><\/li>
- \nRadiation\n<\/a><\/li><\/ul><\/li>
- Summary<\/a><\/li><\/ul><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div>
Heat Transfer<\/h2><\/div>
Everyone knows that a cold water bottle will warm up if we leave it in a hot environment, and if we put the cold water bottle in a refrigerator, the water will become colder. We also know that heat will transfer from areas with high temperature to areas with low temperature. This phenomenon is scientifically called “Heat Transfer”.<\/p>\n<\/div>
The First Law of Thermodynamics<\/h3><\/div>
The first law of thermodynamics is known by the principle of “Conservation of energy,” which states that “energy cannot be created or destroyed, but only transformed into other forms of energy.”<\/p>\n
From this statement, we can write the equation as:<\/p>\n
(Ein<\/sub>) – (Eout<\/sub>) = (\u0394Esystem<\/sub>)<\/p>\n
- \n
- Ein<\/sub> <\/span>= Energy input to the system<\/li>\n
- Eout <\/span><\/sub>= Energy output from the system<\/li>\n
- \u0394Esystem <\/sub>= Energy change in the system<\/li>\n<\/ul>\n<\/div>
<\/span><\/div>Figure 1: Diagram explaining the conservation of energy law with energy input, energy output, and changes\n<\/p><\/div><\/div><\/div>
Energy Balance for Closed Systems<\/h4><\/div>
Closed Systems refers to systems where mass does not change such as a soda can at 12\u00b0C placed at room temperature of 25\u00b0C. Over time, the soda can temperature increases to 20\u00b0C<\/span><\/p>\n
From the example, the soda can has the same mass of water as initially set, but receives heat from the outside environment which has a higher temperature (25\u00b0C), causing the soda can temperature to rise to 20\u00b0C (the water becomes warmer).<\/p>\n
We can write the equation as:<\/p>\n
(Ein<\/sub>) – (Eout<\/sub>) = (\u0394Esystem<\/sub>)<\/p>\n
\u0394U = mcv<\/sub>\u0394T<\/p>\n
or<\/p>\n
Q = mcv<\/sub>\u0394T<\/p>\n
- \n
- \u0394U = <\/span>Energy change in the system, or \u0394Esystem<\/sub><\/li>\n
- Q = <\/span>Heat energy (kJ)<\/li>\n
- m = <\/span>Mass of the system (kg)<\/li>\n
- cv <\/sub>= <\/span>Specific heat capacity (kJ\/kg.K) <\/span><\/sub><\/li>\n
- \u0394T = <\/span>Temperature change (K)<\/li>\n<\/ul>\n<\/div>
<\/span><\/div>Figure 2: Example image of a can and calculations\n<\/p><\/div><\/div><\/div>
Energy Balance for Open Systems (Steady-Flow System)<\/h4><\/div>
Steady-Flow System is a system with constant flow where the mass flowing in equals the mass flowing out, such as a water pipe with water flowing inside, where the water flowing in at the beginning of the pipe equals the water flowing out at the end of the pipe. This system is called a Steady-Flow System.<\/p>\n
We can write the equation as:<\/p>\n
Q\u0307 = \u1e41cv<\/sub>\u0394T<\/p>\n
- \n
- \u0394U = <\/span>Energy change in the system, or \u0394Esystem<\/sub><\/li>\n
- Q\u0307 = <\/span>Heat transfer rate (kJ\/s)<\/li>\n
- \u1e41 = <\/span>Mass flow rate (kg\/s)<\/li>\n
- cv <\/sub>= <\/span>Specific heat capacity (kJ\/kg.K) <\/span><\/sub><\/li>\n
- \u0394T = <\/span>Temperature change (K)<\/li>\n<\/ul>\n<\/div>
<\/span><\/div>Figure 3: Example image of flow inside a pipe<\/p><\/div><\/div><\/div><\/div><\/div><\/div><\/div>
Heat Transfer Mechanisms<\/h3><\/div>
Heat transfer from one area to another can be accomplished in 3 ways:<\/p>\n
- \n
- Conduction<\/li>\n
- Convection<\/li>\n
- Radiation<\/li>\n<\/ol>\n<\/div>
- \n
- Conduction<\/li>\n<\/ul><\/h3><\/div>
Heat transfer that requires a medium including solids, liquids, and gases, where the medium is stationary with a fixed shape.<\/p>\n
For example:<\/p>\n
- \n
- Using metal chopsticks to pick up pork from a pan and feeling heat in your hand, because the metal chopsticks receive heat and transfer the heat to our hand.<\/li>\n
- Static air between building glass is also considered conduction.<\/li>\n<\/ul>\n<\/div><\/span><\/div>
Figure 4: Example image explaining heat conduction with chopsticks and fire<\/p><\/div><\/div><\/div>
Thermal Conductivity or K-Value<\/h4><\/div>
As we know, when eating hot pot, we should use wooden chopsticks instead of metal chopsticks because wooden chopsticks won’t get hot, while metal chopsticks will get hot. Do we know why?<\/p>\n
What makes these two types of chopsticks different is the thermal conductivity (K-Value), which indicates how much heat can be transferred to the other side, depending on the type of material.<\/p>\n
- \n
- If the thermal conductivity coefficient is high, it means it can transfer a lot of heat.<\/li>\n
- If the thermal conductivity coefficient is low, it means it can transfer little heat.<\/li>\n<\/ul>\n<\/div><\/span><\/div>
Figure 5: Image showing the difference between materials with high and low thermal conductivity<\/p><\/div><\/div><\/div>
From the example, we can say that “metal” chopsticks have high thermal conductivity, while “wooden” chopsticks have low thermal conductivity.<\/p>\n
We can calculate the conduction heat transfer rate from:<\/p>\n
Q\u0307cond<\/sub> = kcond<\/sub> x A x (T1<\/sub> -T2<\/sub>) \/\u0394x<\/p>\n
- \n
- Q\u0307cond <\/sub>= Conduction heat transfer rate (kJ\/s)<\/li>\n
- kcond <\/sub>= Thermal conductivity coefficient<\/li>\n
- A = Heat transfer area (m2<\/sup>)<\/li>\n
- T1 <\/sub>= Temperature at point 1 (K)<\/li>\n
- T2 <\/sub>= Temperature at point 2 (K)<\/li>\n
- \u0394x = Thickness of the medium (m)<\/li>\n<\/ul>\n<\/div>
<\/span><\/div>Figure 6: Calculation example with accompanying illustration<\/p><\/div><\/div><\/div>
From this example, we can see that the lower the thermal conductivity coefficient, the lower the temperature on the other side. Therefore, we have another variable called “Thermal Resistance (R-Value)”.<\/p>\n<\/div>
Thermal Resistance or R-Value<\/h4><\/div>
A variable that is opposite to the thermal conductivity coefficient (K-Value).<\/span><\/p>\n
- \n
- If thermal resistance is high, it means the medium allows little heat to pass through.<\/li>\n
- If thermal resistance is low, it means the medium allows a lot of heat to pass through.<\/li>\n<\/ul>\n<\/div>
- \n
- Convection<\/li>\n<\/ul><\/h3><\/div>
The convection process is a process that relies on moving mediums, including liquids and gases, where the high-temperature part rises to the top and the low-temperature part sinks to the bottom, as we often hear “hot air rises, cold air sinks”.<\/p>\n
For example:<\/p>\n
- \n
- Tea boiling in a glass, where we can see tea leaves swirling vertically.<\/li>\n
- Air from an air compressor, which is quite hot.<\/li>\n<\/ul>\n<\/div><\/span><\/div>
Image of heat convection in a tea cup<\/p><\/div><\/div><\/div>
Convection depends on the characteristics of heat convection. For cold air, we can classify it as:<\/p>\n
- \n
- Free Convection (Natural Convection)<\/li>\n
- Forced Convection<\/li>\n<\/ol>\n
For example, on a very hot day after exercising, if we stay still, we call it “Free Convection,” but if we say it’s too hot and need to turn on a fan, we call it “Forced Convection”.<\/p>\n<\/div>
<\/span><\/div>Figure 7: Image of Free Convection and Forced Convection<\/p><\/div><\/div><\/div>
Convection Coefficient<\/h4><\/div>
This variable tells us how much heat the environment at that moment can convect away.<\/p>\n
- \n
- If the convection coefficient is high, it means the fluid can carry away a lot of heat.<\/li>\n
- If the convection coefficient is low, it means the fluid can carry away little heat.<\/li>\n<\/ul>\n<\/div><\/span><\/div>
Figure 8: Image of fluids that can carry away different amounts of heat<\/p><\/div><\/div><\/div>
We can calculate the heat transfer rate from convection using Newton’s law of cooling:<\/p>\n
Q\u0307conv<\/sub> = hconv <\/sub>As <\/sub>(Ts<\/sub> -T\u221e<\/sub>)<\/p>\n
- \n
- Q\u0307conv <\/sub>= Convection heat transfer rate (kJ\/s)<\/li>\n
- h<\/span>conv <\/sub>= Convection coefficient<\/li>\n
- As<\/sub> = Surface area where convection occurs (m2<\/sup>)<\/li>\n
- Ts <\/sub>= Object surface temperature (K)<\/li>\n
- T\u221e <\/sub>= Fluid temperature (K)<\/li>\n<\/ul>\n<\/div>
<\/span><\/div>Figure 9: Image of heat convection calculation<\/p><\/div><\/div><\/div>
From this example, we can say that the amount of heat through convection depends on the values of:<\/p>\n
- \n
- h<\/span>conv <\/sub>Convection coefficient<\/li>\n
- As <\/sub>Surface area<\/li>\n
- T\u221e <\/sub>Fluid temperature<\/li>\n<\/ol>\n<\/div>
- \n
- Radiation<\/li>\n<\/ul><\/h3><\/div>
- As <\/sub>Surface area<\/li>\n
- h<\/span>conv <\/sub>= Convection coefficient<\/li>\n
- Q\u0307conv <\/sub>= Convection heat transfer rate (kJ\/s)<\/li>\n
- Convection<\/li>\n<\/ul><\/h3><\/div>
- kcond <\/sub>= Thermal conductivity coefficient<\/li>\n
- Q\u0307cond <\/sub>= Conduction heat transfer rate (kJ\/s)<\/li>\n
- Conduction<\/li>\n<\/ul><\/h3><\/div>
- Q\u0307 = <\/span>Heat transfer rate (kJ\/s)<\/li>\n
- Q = <\/span>Heat energy (kJ)<\/li>\n
- Eout <\/span><\/sub>= Energy output from the system<\/li>\n
- Heat Transfer Mechanisms<\/a><\/li>
- The First Law of Thermodynamics<\/a><\/li>