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[Audio] What is happening? Let say that we have a lovely cup of milo placed in a room-temperature room.. 

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Let say that we have a lovely cup of milo placed in a  room-temperature room.

[Audio] What is happening? After a while, the hot milo is no longer hot and have the same degree of hotness as the room. So what is happening here?
When we placed the hot milo in the room, we know that after a while, the hot milo will be in some kind of thermal equilibrium with the room. Heat leaves and enters the milo at the same rate. In other words, there is no net flow of heat between the milo and the environment. We refer this equilibrium as thermal equilibrium. 

Scene 3

After a while, the hot milo is no longer hot and have the same degree of 
hotness as the room. So what is happening here?
When we placed the hot milo in the room, we know that after a while, the 
hot milo will be in some kind of thermal equilibrium with the room. Heat 
leaves and enters the milo at the same rate. In other words, there is no net 
flow of heat between the milo and the environment. We refer this 
equilibrium as thermal equilibrium

[Audio] Temperature Previously we looked at a two bodies system that involves a cup of hot milo and a room. Let say we have a three bodies system. If two of the bodies are in thermal equilibrium with the third body, they must be in thermal equilibrium with each other. This is the zeroth law of thermodynamic.. 

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Previously we looked at a two bodies system that involves a cup of  hot milo and a room. Let say we have a three bodies system.


 If two of the bodies are in thermal equilibrium with the  third body, they must be in thermal equilibrium with each other.  This is the zeroth law of thermodynamic.

[Audio] Temperature is describe as the degree of hotness, used to describe a physical property to determine whether or not two objects are in thermal equilibrium. How can we measure temperature? What can we use to measure temperature?. 

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Temperature is describe as the degree of hotness, used to  describe a physical property to determine whether or not  two objects are in thermal equilibrium. How can we measure temperature? What can we use to  measure temperature?

[Audio] Making a Thermometer How do we make thermometer in the first place? How do we know that 300C is indeed 300C? The idea of thermometer originate from the concept that there are some materials responds to temperature. In other words, the properties. Recall back to the topic on ideal gases. Charles’s law states that the volume of a gas is proportional to the temperature. Thus the volume expands when the temperature increases and vice versa. 

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How do we make thermometer in the first place? How do  we know that 300C is indeed 300C? The idea of thermometer originate from the concept that  there are some materials responds to temperature. In  other words, the properties. Recall back to the topic on  ideal gases. Charles’s law states that the volume of a gas  is proportional to the temperature. Thus the volume expands  when the temperature increases and vice versa

[Audio] So what material and properties can we use to make thermometer and how can we determine the temperature?. 

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So what material and properties can we use to make  thermometer and how can we determine the  temperature?

[Audio] Number 1 – The materials and properties that are suitable to make a thermometer. Metals – expansions of material with temperature. Metals – the resistance of the material will vary with temperature. Gas – the kinetic energy increases with increase in temperature. Thus the volume increases. This is illustrated with Charles’s Law, V α T These materials are known as thermometric substances. 

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Number 1 – The materials and properties that are suitable  to make a thermometer. Metals – expansions of material with temperature. Metals – the resistance of the material will vary with temperature. Gas – the kinetic energy increases with increase in temperature. Thus the volume increases. This is illustrated with Charles’s Law, V α T. These materials are known as thermometric substances

[Audio] Number 2 – How to make use of the properties to make a thermometer? We know that the properties discussed earlier vary with temperature but we still need to know how to use the properties to make a thermometer. How can we know the temperature of a body?. 

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Number 2 – How to make use of the properties to make a  thermometer? We know that the properties discussed earlier vary with  temperature but we still need to know how to use the  properties to make a thermometer. How can we know the  temperature of a body?

[Audio] Number 2 – How to make use of the properties to make a thermometer? We cannot tell what temperature a body has at any one time because we have no reference line. However we do know two points when it comes to water. We know that it freezes at one point and boils at one point. We can make use of the two points and make it as reference points. 

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Number 2 – How to make use of the properties to make a  thermometer? We cannot tell what temperature a body has at any one  time because we have no reference line. However we do  know two points when it comes to water. We know that it  freezes at one point and boils at one point. We can make  use of the two points and make it as reference points

[Audio] Number 2 – How to make use of the properties to make a thermometer? We now have taken two reference points. In Celsius scale, the point at which water freezes is 00C and the point at which water boils is 1000C. Any other points between or beyond the two points may be calculated by cross multiply. 

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Number 2 – How to make use of the properties to make a  thermometer? We now have taken two reference points. In Celsius scale,  the point at which water freezes is 00C and the point at  which water boils is 1000C. Any other points between or  beyond the two points may be calculated by cross- multiply

[Audio] Lets have a look at a liquid metal – mercury. It expands with increase in temperature and vice versa. We then put it to a scale. If we put in a metre scale, we have,. 

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Lets have a look at a liquid metal – mercury. It expands  with increase in temperature and vice versa. We then put  it to a scale. If we put in a metre scale, we have,

[Audio] (steam point) XS 1000C Xt t0C (ice point) 00C Xi. 

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[Audio] Assuming X varies uniformly or linearly, with temperature measured, therefore. 

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Assuming X varies uniformly or linearly, with temperature  measured, therefore

[Audio] Thermometer. Thermometer. capillary tube graduation mercury in bore of tube bulb sliding maximum marker. 

Scene 15

capillary tube
graduation
mercury in
bore of tube
bulb
sliding
maximum
marker

Scene 16

Thermometer. ua;aLLIOLU-1eq-; se6 euri10A 41-EJSUOO. 

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Thermometer. Current sensor ice Heat source Temperature sensor Water. 

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Current sensor
ice
Heat source
Temperature sensor
Water

[Audio] Steam point 1000C Ice point 00C Room temperature Resistance of resistance thermometer 75.000 ohms 63.000 ohms 64.992 ohms Pressure recorded by constant volume gas thermometer 1.10 x 107 Nm-2 8.00 x 106 Nm-2 8.51 x 106 Nm-2 Using the data given above, calculate the room temperature on both the thermometers.. 

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Steam point 1000C Ice point 00C Room temperature Resistance of resistance thermometer 75.000 ohms 63.000 ohms 64.992 ohms Pressure recorded by constant volume gas thermometer 1.10 x 107 Nm-2 8.00 x 106 Nm-2 8.51 x 106 Nm-2

Using the data given above, calculate the room temperature on both the thermometers.

[Audio] The Absolute Thermodynamic Scale
We first deal with the Celsius scale. How about the Kelvin scale that is the SI unit in physics?
This scale is based on the ideal gas equation, PV proportional to T, which shows a linear relation for the thermometric parameters of P, V and T Similar procedure as before, we need two points as references.. 

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We first deal with the Celsius scale. How about the Kelvin 
scale that is the SI unit in physics?
This scale is based on the ideal gas equation, PV 
proportional to T, which shows a linear relation for the 
thermometric parameters of P, V and T.
Similar procedure as before, we need two points as 
references.

[Audio] So what suitable points can we use? The points that can be use are 1. Lower fixed point – absolute zero, obtained from PV α T 2. Upper fixed point – triple point temperature of water.. 

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So what suitable points can we use? The points that can be  use are 1. Lower fixed point – absolute zero, obtained from PV α T 2. Upper fixed point – triple point temperature of water.

[Audio] Triple point of Water The triple point of water, Ttr , is the temperature at which saturated water vapour, pure water and ice all coexist in equilibrium. It is better reference point as it is unique and invariant. A value of 273.16 K is assigned to the triple point of water. (The kelvin is the SI unit for the fundamental temperature. It is defined as the fraction 1/273.16 of the thermodynamic temperature of the triple point of water. 

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The triple point of water, Ttr , is the temperature at which  saturated water vapour, pure water and ice all coexist in  equilibrium. It is better reference point as it is unique and  invariant. A value of 273.16 K is assigned to the triple  point of water. (The kelvin is the SI unit for the  fundamental temperature. It is defined as the fraction  1/273.16 of the thermodynamic temperature of the triple point  of water

[Audio] The Absolute Thermodynamic Scale At the triple point of water, Ttr At a general temperature. T Therefore,. 

Scene 23

At the triple point of water, Ttr
 At a general temperature. T

 Therefore,

Temperature

avatar

What is happening?
 Let say that we have a lovely cup of milo placed in a  room-temperature room.

What is happening? 
After a while, the hot milo is no longer hot and have the same degree of 
hotness as the room. So what is happening here?
When we placed the hot milo in the room, we know that after a while, the 
hot milo will be in some kind of thermal equilibrium with the room. Heat 
leaves and enters the milo at the same rate. In other words, there is no net 
flow of heat between the milo and the environment. We refer this 
equilibrium as thermal equilibrium

Temperature
 Previously we looked at a two bodies system that involves a cup of  hot milo and a room. Let say we have a three bodies system.


 If two of the bodies are in thermal equilibrium with the  third body, they must be in thermal equilibrium with each other.  This is the zeroth law of thermodynamic.

Making a Thermometer
 How do we make thermometer in the first place? How do  we know that 300C is indeed 300C? The idea of thermometer originate from the concept that  there are some materials responds to temperature. In  other words, the properties. Recall back to the topic on  ideal gases. Charles’s law states that the volume of a gas  is proportional to the temperature. Thus the volume expands  when the temperature increases and vice versa

Number 1 – The materials and properties that are suitable  to make a thermometer. Metals – expansions of material with temperature. Metals – the resistance of the material will vary with temperature. Gas – the kinetic energy increases with increase in temperature. Thus the volume increases. This is illustrated with Charles’s Law, V α T These materials are known as thermometric substances

Number 2 – How to make use of the properties to make a  thermometer? We now have taken two reference points. In Celsius scale,  the point at which water freezes is 00C and the point at  which water boils is 1000C. Any other points between or  beyond the two points may be calculated by cross multiply

(steam point)
 XS
 1000C
 Xt
 t0C
 (ice point)
 00C
 Xi

Steam point 1000C Ice point 00C Room temperature Resistance of resistance thermometer 75.000 ohms 63.000 ohms 64.992 ohms Pressure recorded by constant volume gas thermometer 1.10 x 107 Nm-2 8.00 x 106 Nm-2 8.51 x 106 Nm-2
 Using the data given above, calculate the room temperature on both the thermometers.

The Absolute Thermodynamic Scale
We first deal with the Celsius scale. How about the Kelvin 
scale that is the SI unit in physics?
This scale is based on the ideal gas equation, PV 
proportional to T, which shows a linear relation for the 
thermometric parameters of P, V and T Similar procedure as before, we need two points as 
references.

Triple point of Water
 The triple point of water, Ttr , is the temperature at which  saturated water vapour, pure water and ice all coexist in  equilibrium. It is better reference point as it is unique and  invariant. A value of 273.16 K is assigned to the triple  point of water. (The kelvin is the SI unit for the  fundamental temperature. It is defined as the fraction  1/273.16 of the thermodynamic temperature of the triple point  of water

The Absolute Thermodynamic Scale
 At the triple point of water, Ttr
 At a general temperature. T

 Therefore,