
| Equation: | 
              Description: | 
            
| Conservation of Energy Principle | 
            |
| For a cycle, the initial and final state
                of the system are the same and thus have the same amount
                of energy. | 
            |
| Because there is no change in energy
                between the initial and final states of the cycle, all
                added energy must leave within the same cycle. | 
            |
| The only energy added to the system in
                heat from the Hot Reservoir. | 
            |
| Energy leaves the cycle at the cold
                reservoir and in the form of work. (Ideally only in
                those two forms, in reality it would include far more
                forms). | 
            |
| Rearranging the energy balance, these are
                all the ways in which energy is transfer to or from a
                Stirling Engine. | 
            |
| Solving the energy balance for work
                output, in terms of heat transfer in and out. | 
            |
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              Another bit of information one might be
                interested in is the thermal efficiency (ηth)
                
                
                
                
                
                
                
                
                
                 of the Stirling
                Engine. | 
            
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              Theoretically, the highest efficiency for
                a heat engine is the Carnot Efficiency, which can be
                calculated if one knows the absolute temperatures of the
                hot and cold reservoirs | 
            
From the above, one can, knowing a few values determine the
          work a Stirling engine can produce, how efficient it is and
          compare its efficiency to the maximum efficiency that a heat
          engine can have given the temperature of its' reservoirs.
        
The math above applies to all Stirling Engines, so if you'd
          like to learn about the variations, click here.
        
        
        
Professor: David Newman, Ph.D.
            Course: PHYS 212
            Semester: Spring 2017
            Student: Riley Bickford