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 fixed a problem 20250919, metal cup has to lose heat faster than porcelain, thank to K Raman

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http://iwant2study.org/lookangejss/03thermalphysics_11thermalpropertiesofmatter/ejss_model_cooling/cooling_Simulation.xhtml

Briefing Document: 🌡️Block Mass Cooling and Heating Curve Simulation

1. Overview:

This document analyzes a simulation model focusing on heat transfer, specifically the cooling and heating of a block of various materials. The model, developed using Easy JavaScript Simulations (EJS), allows users to explore the principles of thermal physics, particularly Newton's Law of Cooling, and the effects of different materials and surface areas on heat transfer rates. This resource is intended for secondary and junior college level physics education and is accessible on various platforms including computers and mobile devices. The simulation is a valuable tool for visualizing and understanding concepts related to heat conduction, specific heat capacity, and thermal equilibrium.

2. Main Themes and Key Concepts

A = 6 (\frac{m}{\rho})^{\frac{2}{3}} and A_{increased surface area due to fins} = (2)(6) (\frac{m}{\rho})^{\frac{2}{3}}

3. Important Facts and Ideas

4. Quotes

5. Educational Value:

6. Limitations:

7. Conclusion

The "Block Mass 0.1 kg Cooling and Heating Curve with Different Materials and Surface Area Model" provides a valuable, interactive resource for learning about heat transfer, Newton’s Law of Cooling, and the impact of material properties on thermal behavior. The model, along with its underlying equations, offers a practical approach for understanding complex heat transfer concepts. While it simplifies some aspects of real-world heat transfer, it serves as an excellent tool for developing a fundamental understanding of thermal physics concepts. The inclusion of various materials, surface finishes, and the ability to apply heating make the simulation a powerful educational asset.

 

Thermal Physics Study Guide

Quiz

Instructions: Answer the following questions in 2-3 sentences each.

  1. According to the simulation, how does the material of an object affect its rate of cooling?
  2. What is the key assumption made by the Newton's Law of Cooling model regarding temperature within an object?
  3. What does the heat transfer coefficient represent, and how does it differ between shiny and dull surfaces in the simulation?
  4. How is the surface area of the cube calculated in this simulation, and what happens when fins are added?
  5. What is specific heat capacity, and how does it relate to the amount of energy required to change an object's temperature?
  6. Explain the concept of thermal equilibrium in the context of this simulation.
  7. How does the simulation model the impact of heating, and how does this affect the final ordinary differential equation (ODE)?
  8. Describe how the simulation can be used to explore and compare the thermal properties of different materials.
  9. In the context of the simulation and the experiment described, what does it mean for a material to be a good conductor?
  10. What factors, not explicitly included in the simulation, might influence the actual value of the heat transfer coefficient?

Quiz Answer Key

  1. The material of the object significantly impacts its cooling rate; good conductors of heat, like metals, lose heat faster than poor conductors, like wood or porcelain. Different materials have different specific heat capacities and thermal conductivity, which dictates how quickly they transfer heat.
  2. The Newton's Law of Cooling model assumes that the temperature within the object is uniform at any given time. This means the model is treating the entire object as a single 'lump' with one temperature instead of accounting for different temperatures within the object.
  3. The heat transfer coefficient (h) indicates how effectively heat is transferred between an object and its surroundings; shiny surfaces have a higher coefficient (400 W/(K m²)) than dull surfaces (200 W/(K m²)) in this simulation, representing their greater ability to transfer heat.
  4. The surface area (A) of the cube is calculated using the formula A = 6(m/ρ)^(2/3), assuming a cubic shape. The inclusion of fins doubles this surface area, increasing it by a factor of two, which increases the cooling or heating.
  5. Specific heat capacity (c) is the amount of heat energy (Q) needed to raise the temperature of one kilogram of a substance by one degree Celsius (or Kelvin); a material with a high specific heat capacity requires more energy to achieve the same temperature change than a material with low specific heat capacity.
  6. Thermal equilibrium is reached when there is no more net heat transfer between the object and its surroundings because they have the same temperature. In the simulation, this is the point where the object's temperature becomes constant over time.
  7. The simulation models heating as an additional term in the final ODE that is added to the cooling equation, representing an input of thermal energy. This heating term affects the object's temperature changes, opposing cooling, and is proportional to the heating input and inversely proportional to the product of mc.
  8. The simulation allows users to change parameters such as the material and its surface, observing how the temperature changes over time. This helps users to compare how different materials heat or cool under the same conditions and how these changes are represented on the graph.
  9. In the context of the simulation, a good conductor is a material that quickly transfers heat to or from its surroundings. This means it will cool down much faster when it is hotter than its surroundings.
  10. The heat transfer coefficient is affected by factors such as the fluid velocity, viscosity, surface roughness of the object and fluid, and external flow conditions like turbulent or laminar flow, all of which are not explicitly modeled within the simulation and are simply assigned specific constant values.

Essay Questions

Instructions: Answer the following questions using information from the provided source material.

  1. Discuss the practical implications of Newton's Law of Cooling, using examples from everyday life and considering the limitations of the model.
  2. Compare and contrast how the material properties and surface conditions of an object affect its heat transfer rate, using evidence from the simulation and the given information about the heat transfer coefficient.
  3. Describe the mathematical model that underlies the simulation of thermal processes, explaining the role of each parameter and the assumptions used to simplify the model.
  4. Analyze how the specific heat capacity and the density of a material affect the rate of its temperature change when it's heated or cooled, and discuss how these properties are factored into the simulation.
  5. Explore the educational value of the simulation, explaining how it can aid in understanding heat transfer concepts and the importance of experimental assumptions in scientific modeling.

Glossary of Key Terms

Sample Learning Goals

1) compare how conductors of heat lose heat or gain heat
2) explain how conductors of heat play an important part in our lives

SLS Lesson by Kong Su Sze

Good conductors of heat

steel, copper

Poor conductors of heat

plastic, wood

The beginning temperature of the hot water in both cups is ◦c. The room temperature of the experiment is ◦c. 
Both the temperature of the hot water in the 2 cups drop over time. The temperature of the hot water in the metal cup drops  than the temperature of the hot water in the porcelain cup.  The hot water in the metal cup heat to the surrounding . The water in the metal cup takes a  time to reach 30 ◦c compared to the water in the porcelain cup.
 
We can conclude that metal is a conductor of heat while porcelain is a conductor of heat.
The temperature of the water in both cups remain constant after a while because there is no heat transfer between the and the .

Answer Key

 

For Teachers

Newton's Law of Cooling


The Newton's Law of Cooling model computes the temperature of an object of mass M as it is heated or cooled by the surrounding medium.

 

Assumption:

The model assumes that the temperature T within the object is uniform. 

Validity:

 This lumped system approximation is valid if the rate of thermal energy transfer within the object is faster than the rate of thermal energy transfer at the surface. 

Convection-cooling "Newton's law of cooling" Model:

Newton assumed that the rate of thermal energy transfer at the object's surface is proportional to the surface area and to the temperature difference between the object and the surrounding medium. 

\( \frac{\delta Q}{\delta t} = h A( T(t) - T_{background} )\)
 
\( Q \) is the thermal energy in joules
\( h \) is the heat transfer coefficient (assumed independent of T here) (\(\frac{W}{m^{2} K}\))
\( A \) is the heat transfer surface area (\( m^{2} \))
\( T \) is the temperature of the object's surface and interior (since these are the same in this approximation)
\( T_{background} \) is the temperature of the surrounding background environment; i.e. the temperature suitably far from the surface is the time-dependent thermal gradient between environment and object.

Definition Specific Heat Capacity:

The specific heat capacity of a material on a per mass basis is
 
\( Q = mc ( T_{final} - T_{initial} ) \)
\( Q \) is heat energy 
\( m \)  is the mass of the body
\( c \) specific heat capacity of a material
\( T_{final} \) is the \(T_{background}\)
\( T_{initial}\) is the \( T(t) \) 
 
 
combing the 2 equations

\( \frac{mc ( T_{background}- T(t) ) }{\delta t} = h A( T(t) - T_{background} )\)

assuming mc is constant'

\( mc \frac{ \delta ( T_{background}- T(t) ) }{\delta t} = h A( T(t) - T_{background} )\)

assuming \(T_{background}\) is a infinite reservoir

\( \frac{ ( T_{background}) }{\delta t} = 0 \)
therefore
\( mc \frac{ ( \delta (- T(t)) ) }{\delta t} = h A( T(t) - T_{background} )\)

negative sign can be taken out of the differential equation.

\( mc \frac{ (\delta T(t) ) }{\delta t} =  -h A( T(t) - T_{background} )\)
 
\( \frac{ ( T(t) ) }{\delta t} =  -\frac{h A}{mc }( T(t) - T_{background} )\)

let \( \kappa  = \frac{h A}{mc } \)

\( \frac{ ( T(t) ) }{\delta t} = -\kappa ( T(t) - T_{background} )\)

If heating is added on,

\( heating = \frac{\delta Q}{\delta t} = mc ( \frac{\delta T}{\delta t}) \)

the final ODE equation looks like

\( \frac{ ( T(t) ) }{\delta t} = -\kappa ( T(t) - T_{background} ) + \frac{heating}{mc}\)

Definition Equation Used:

\( V = \frac{m}{\rho} \)

\( V \) is volume of object
\( \rho \) is density of object


\( A = 6 (\frac{m}{\rho})^{\frac{2}{3}} \)

\( A \) surface area of object

assumption of increased surface are

\( A_{increased surface area due to fins} = (2)(6) (\frac{m}{\rho})^{\frac{2}{3}} \)

Materials added:

copper shiny \( c_{Cu} \) = 385  \( \frac{J}{kg K}\)
\( \rho_{Cu} \) = 8933  \( \frac{kg}{m^{3}}\)
heat transfer coefficient  \(h_{Cu}\) = 400 \( \frac{W}{(K m^{2})} \)

copper dull \( c_{Cu} \) = 385  \( \frac{J}{kg K}\)
\( \rho_{Cu} \) = 8933  \( \frac{kg}{m^{3}}\)
heat transfer coefficient  \(h_{Cu}\) = 200 \( \frac{W}{(K m^{2})} \)

aluminium shiny \( c_{Al} \) = 903  \( \frac{J}{kg K}\)
\( \rho_{Al} \) = 2702  \( \frac{kg}{m^{3}}\)
heat transfer coefficient  \(h_{Al}\) = 400 \( \frac{W}{(K m^{2})} \)

aluminium dull \( c_{Al} \) =  903  \( \frac{J}{kg K}\)
\( \rho_{Al} \) = 2702  \( \frac{kg}{m^{3}}\)
heat transfer coefficient  \(h_{Al}\) = 200 \( \frac{W}{(K m^{2})} \)

iron shiny \( c_{Al} \) = 447  \( \frac{J}{kg K}\)
\( \rho_{Al} \) = 7870  \( \frac{kg}{m^{3}}\)
heat transfer coefficient  \(h_{Al}\) = 400 \( \frac{W}{(K m^{2})} \)

iron dull \( c_{Al} \) =  447  \( \frac{J}{kg K}\)
\( \rho_{Al} \) = 7870  \( \frac{kg}{m^{3}}\)
heat transfer coefficient  \(h_{Al}\) = 200 \( \frac{W}{(K m^{2})} \)
 

Users can select the mass of the object and the material and the model computes the surface area assuming a cubic shape. The model plots the object's temperature as a function of time as the user heats and cools the object. A data-tool button on the temperature graph allows users fit the data to analytic functions. 


Note: A typical (rough) heat transfer coefficient h for still air and iron is 6 W/(K m^2) and 400 W/(K m^2) . The Newton's Law of Cooling model assumes h=400 for all shiny and h=200 for dull materials. The actual value of h depends on many parameters including the material, the fluid velocity, the fluid viscosity and the condition of the object's surface. 

References:


  1. "Measuring the Specific Heat of Metals by Cooling," William Dittrich, The Physics Teacher, (in press).

Credits:

  1. The Newton's Law of Cooling model was created by Wolfgang Christian using the Easy Java Simulations (EJS) version 4.2 authoring and modeling tool.
  2. EJSS Cube Block Cooling Model was created by Wolfgang Christian and recreated by lookang using the Easy Java Simulations (EJS) version 5.1 authoring and modeling tool

Research

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Video

 

https://www.youtube.com/watch?v=8a8nTQIdLOM {source}<iframe width="560" height="315" src="https://www.youtube.com/embed/8a8nTQIdLOM" title="YouTube video player" frameborder="0" allow="accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture" allowfullscreen></iframe>{/source}

 Version:

  1. http://weelookang.blogspot.sg/2014/11/ejss-cube-block-cooling-model.html 
  2. https://vle.learning.moe.edu.sg/community-gallery/lesson/view/5d907c47-4ae6-47e7-8cce-04199b1cd386

Hands-On Kits

  1. http://www.addest.com/products/category/Science_Kits by Addest Station Cooling Curve Kit Cooling Curve Kit

Other Resources

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FAQ on Heat Transfer and Material Properties

The density (ρ) of a material is crucial when calculating the surface area of an object, especially when considering shapes like cubes. The surface area is calculated as A = 6*(m/ρ)^(2/3), where m is the mass and ρ is the density of the material. A denser material will result in a smaller surface area for a given mass, thus impacting the rate of heat transfer. Materials with higher density will have less surface area for the same mass.

Parent Category: 13 Thermodynamic Systems
Category: 04 Thermal Properties of Matter
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