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Thermal Flow If you can’t stand the heat. Temperature  As we know Temperature is the average kinetic energy of the molecules. As they bounce around they.

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Presentation on theme: "Thermal Flow If you can’t stand the heat. Temperature  As we know Temperature is the average kinetic energy of the molecules. As they bounce around they."— Presentation transcript:

1 Thermal Flow If you can’t stand the heat

2 Temperature  As we know Temperature is the average kinetic energy of the molecules. As they bounce around they exchange energy.  Transfer of heat between liquids and gas’s are easy to see since the molecules are relatively free to move. But for a solid the energy transfer is less about it flying around and more about it’s vibration.

3 Balancing it all out.  The flow of energy in any system is always from high to low. Just like when we pour water on a hill the water wants to go to the lowest point it can.  The same can be said of heat. Heat will always travel from ‘hot’ to ‘cold’ and never the other way around.  It will flow untill it is ‘balanced’ or ‘at equilibrium’ with it’s surroundings. (e.g. the water flowing down the hill ended up in a lake. The water can not go lower down the hill)

4 Flow of heat  Convection: When heat flows between gas or liquid  As the air or the liquid increases in temperature the ‘hotter’ portion moves upwards (hot air rises) away from the heating source and cooling where it falls back down.  Example: your convection oven.

5 Heat flow  Conduction: the transfer of heat from direct contact between 2 objects.

6 Heat flow  Radiation: does not use matter to transfer the heat. Think of the Sun heating the Earth. There is nothing between the Earth and the Sun but we still feel its warmth.

7 Thermal energy conservation  Just like with momentum and energy thermal energy can be conserved.  So if we take 2 blocks one at ‘hot’ and one at ‘cold’ what do you think will happen?

8 Heat flow  We will get ‘warm’  The change in the first blocks heat will equal the change in the 2 nd blocks heat just in reverse.  So basically Q lost = Q gain  Or as the law of conservation states, there should be no loss so they should sum up to zero.  Q 1 + Q 2 = 0 (remember one is losing heat so it will be negative)

9 Example  A 29.5kg sample of methanol at 208.9 K is mixed with 54.3kg of methanol at 302.3 K. Calculate the final tempeerature if the specific heat of methanol is 2.53 J/kgK  (mass) (Δt) (C p ) = (mass) (Δt) (C p )  Q lost on the left; Q gain on the right.  Substituting and solving, we have:  (29.5) (x - 208.9) (2.53) = (54.3) (302.3 - x) (2.53)  29.5x - 6162.55 = 16414.89 - 54.3x  83.8x = 22577.44  X = 269.4K

10 Background  This method was used to determine the specific heat of different object.  They would take a calorimeter and put in the substance. Then measure the change in the temperature.


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