chapter 6.6 & 6.7 entropy and specific heat
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Chapter 6.6 & 6.7 Entropy and Specific Heat. Why is it that the filling of a hot apple pie may be too hot to eat, even though the crust is not?. Entropy. 1 st law- quantity of energy 2 nd law- quality of energy - PowerPoint PPT PresentationTRANSCRIPT
Chapter 6.6 & 6.7 Entropy and Specific Heat
Why is it that the filling of a hot apple pie may be too hot to eat,
even though the crust is not?
Entropy
• 1st law- quantity of energy
• 2nd law- quality of energy– A further definition of 2nd law: In natural
processes, high-quality energy tends to transform into lower quality energy.
– A process in which disorder returns to order without external help does not occur
Entropy
• And as time increases…….disorder does too
• Time always points in the direction from order to disorder– Old movies with damsel in distress tied to a
train track.– Next time look for the telltale signs of the
smoke entering the smokestack
Entropy
• The idea of ordered energy tending to disordered energy is the concept of entropy
• Entropy is the measure of how energy spreads to disorder in a system
• When disorder increases- entropy increases– The heat from a camp fire cannot spontaneously
return to the fire and restore the firewood to its original state.
– The molecules of an automobiles exhaust cannot recombine to form highly organized gasoline molecules.
Entropy
• When ever a system is allowed to spread its energy freely, it always does so in a manner that increases entropy (disorder)
• But energy can be put into a system in the form of WORK. – Living organisms extract energy from their
surroundings and use this energy to increase their own organization
– This decreases the entropy of the living organism’s system
– Plants extract photons of light for energy and create glucose through photosynthesis.
Entropy
• Even though the entropy of a living organisms may decrease
• It does so by increasing the entropy of its surroundings.
• So life forms plus their waist products have a net increase in entropy.
• Energy must be transformed within a living system
• When it cannot, the organism soon dies and again tends toward disorder.
Specific Heat Capacity
• Opening question…discussion• Some foods remain hotter longer than others. • Different substances have different thermal
capacities for storing heat. – Water, iron, and silver– Equal masses of different substances require a
different quantity of heat to change their temperatures by a specific number of degrees.
– Recall calories…. 1g of water needs 1cal of energy to raise the temp 1 degree C.
Specific Heat Capacity
• We consider water to have higher specific heat capacity (often called specific heat for short) – The specific heat capacity of any
substance is defined as the quantity of heat required to change the temperature of a unit mass of the substance by 1 degree Celsius.
Specific Heat Capacity
• A great way to think of specific heat capacity is by thinking of it as thermal inertia
• Mathematically explaining specific heat– The specific heat of a substance can be calculated if
you know how much heat is put into the material and how much the material changes temperature.
– Q= cmΔT – Q is the quantity of heat– c is the specific heat– m is the mass of the object– ΔT is the change in temperature. Remember: Tf - Ti
Practice Problem A
• Aluminum has a specific heat of 0.902 J/g x 0C. How much heat is lost when a piece of aluminum with a mass of 23.984 g cools from a temperature of 415.0 oC to a temperature of 22.0 oC?– Solve for Q.. How much heat?– Q= cmΔT
Practice Problem A
– Solve for Q.. How much heat?
– Q= cmΔT
– Q= (0.902 J/g x 0C)(23.984g)(22.0 oC - 415.0 oC)=
– Q= 8.50 x 103 J (use correct sigfigs and scientific notation)
Practice Problem B
• mass (m) is the unknown:
• The temperature of a sample of water increases by 69.5 oC when 24 500 J are applied. The specific heat of liquid water is 4.18 J/g x oC. What is the mass of the sample of water?
Practice Problem B
– Solve for m: Q= cmΔT then, m=Q/(c ΔT)
– m = 24 500 J/69.5 oC x 4.18 J/g x oC
– m = 84.3 g
Practice Problem C
• Specific Heat (c) is the unknown:
• When 34 700 J of heat are applied to a 350 g sample of an unknown material the temperature rises from 22.0 oC to 173.0 oC. What must be the specific heat of this material?
Practice Problem C
• Solve for c: Q= cmΔT then, c=Q/(mΔT)• Cp = 34 700 J/350 g x 151.0 oC
• Cp = 0.66 J/g x oC