Carnot method

The Carnot method is an allocation procedure for dividing up fuel input (primary energy, end energy) in joint production processes that generate two or more energy products in one process (e.g. cogeneration or trigeneration). It is also suited to allocate other streams such as CO₂-emissions or variable costs. The potential to provide physical work (exergy) is used as the distribution key. For heat this potential can be assessed the Carnot efficiency. Thus, the Carnot method is a form of an exergetic allocation method. It uses mean heat grid temperatures at the output of the process as a calculation basis. The Carnot method's advantage is that no external reference values are required to allocate the input to the different output streams; only endogenous process parameters are needed. Thus, the allocation results remain unbiased of assumptions or external reference values that are open for discussion.

The fuel share a_el which is needed to generate the combined product electrical energy W (work) and a_th for the thermal energy H (useful heat) respectively, can be calculated accordingly to the first and second laws of thermodynamics as follows:

a_el= (1 · η_el) / (η_el + η_c · η_th)

a_th= (η_c · η_th) / (η_el + η_c · η_th)

Note: a_el + a_th = 1

with
a_el: allocation factor for electrical energy, i.e. the share of the fuel input which is allocated to electricity production
a_th: allocation factor for thermal energy, i.e. the share of the fuel input which is allocated to heat production

η_el = W/Q_F
η_th = H/Q_F
W: electrical work
H: useful heat
Q_F: Total heat, fuel or primary energy input

and
η_c: Carnot factor 1-T_i/T_s (Carnot factor for electrical energy is 1)
T_i: lower temperature, inferior (ambient)
T_s: upper temperature, superior (useful heat)

In heating systems, a good approximation for the upper temperature is the average between forward and return flow on the distribution side of the heat exchanger.
T_s = (T_FF+T_RF) / 2
or - if more thermodynamic precision is needed - the logarithmic mean temperature^[1] is used
T_s = (T_FF-T_RF) / ln(T_FF/T_RF)
If process steam is delivered which condenses and evaporates at the same temperature, T_s is the temperature of the saturated steam of a given pressure.

The fuel intensity or the fuel factor for electrical energy f_F,el resp. thermal energy f_F,th is the relation of specific input to output.

f_F,el= a_el / η_el = 1 / (η_el + η_c · η_th)

f_F,th= a_th / η_th = η_c / (η_el + η_c · η_th)

To obtain the primary energy factors of cogenerated heat and electricity, the energy prechain needs to be considered.

f_PE,el = f_F,el · f_PE,F
f_PE,th = f_F,th · f_PE,F

with
f_PE,F: primary energy factor of the used fuel

The reciprocal value of the fuel factor (f-intensity) describes the effective efficiency of the assumed sub-process, which in case of CHP is only responsible for electrical or thermal energy generation. This equivalent efficiency corresponds to the effective efficiency of a "virtual boiler" or a "virtual generator" within the CHP plant.

η_{el, eff} = η_el / a_el = 1 / f_F,el
η_{th, eff} = η_th / a_th = 1 / f_F,th

with
η_{el, eff}: effective efficiency of electricity generation within the CHP process
η_{th, eff}: effective efficiency of heat generation within the CHP process

Next to the efficiency factor which describes the quantity of usable end energies, the quality of energy transformation according to the entropy law is also important. With rising entropy, exergy declines. Exergy does not only consider energy but also energy quality. It can be considered a product of both. Therefore any energy transformation should also be assessed according to its exergetic efficiency or loss ratios. The quality of the product "thermal energy" is fundamentally determined by the mean temperature level at which this heat is delivered. Hence, the exergetic efficiency η_x describes how much of the fuel's potential to generate physical work remains in the joint energy products. With cogeneration the result is the following relation:

η_x,total = η_el + η_c · η_th

The allocation with the Carnot method always results in:
η_x,total = η_x,el = η_x,th

with
η_x,total = exergetic efficiency of the combined process
η_x,el = exergetic efficiency of the virtual electricity-only process
η_x,th = exergetic efficiency of the virtual heat-only process

The main application area of this method is cogeneration, but it can also be applied to other processes generating a joint products, such as a chiller generating cold and producing waste heat which could be used for low temperature heat demand, or a refinery with different liquid fuels plus heat as an output.

Let's assume a joint production with Input I and a first output O₁ and a second output O₂. f is a factor for rating the relevant product in the domain of primary energy, or fuel costs, or emissions, etc.

evaluation of the input = evaluation of the output

f_i · I = f₁ · O₁ + f₂ · O₂

The factor for the input f_i and the quantities of I, O₁, and O₂ are known. An equation with two unknowns f₁ and f₂ has to be solved, which is possible with a lot of adequate tuples. As second equation, the physical transformation of product O₁ in O₂ and vice versa is used.

O₁ = η₂₁ · O₂

η₂₁ is the transformation factor from O₂ into O₁, the inverse 1/η₂₁=η₁₂ describes the backward transformation. A reversible transformation is assumed, in order not to favour any of the two directions. Because of the exchangeability of O₁ and O₂, the assessment of the two sides of the equation above with the two factors f₁ and f₂ should therefore result in an equivalent outcome. Output O₂ evaluated with f₂ shall be the same as the amount of O₁ generated from O₂ and evaluated with f₁.

f₁ · (η₂₁ · O₂) = f₂ · O₂

If we put this into the first equation, we see the following steps:

f_i · I = f₁ · O₁ + f₁ · (η₂₁ × O₂)

f_i · I = f₁ · (O₁ + η₂₁ · O₂)

f_i = f₁ · (O₁/I + η₂₁ · O₂/I)

f_i = f₁ · (η₁ + η₂₁ · η₂)

f₁ = f_i / (η₁ + η₂₁ · η₂) or respectively f₂ = η₂₁ · f_i / (η₁ + η₂₁ · η₂)

with η₁ = O₁/I and η₂ = O₂/I

• Cogeneration
• Variable cost
• Power loss factor
• Joint product pricing
• Nicolas Léonard Sadi Carnot
• Second law of thermodynamics

• Marc Rosen: Allocating carbon dioxide emissions from cogeneration systems: descriptions of selected output-based methods, Journal of Cleaner Production, Volume 16, Issue 2, January 2008, p. 171–177.
• Andrej Jentsch: The Carnot-Method for Allocation of Fuel and Emissions, EuroHeat&Power, Vol 12 II, 2015, p. 26-28.
• Andrej Jentsch: A novel exergy-based concept of thermodynamic quality and its application to energy system evaluation and process analysis, dissertation, TU Berlin, 2010.
• Verein Deutscher Ingenieure: VDI-Guideline 4608 Part 2, Energy systems - Combined heat and power - Allocation and evaluation, Juli 2008.
• EN 15316-4-5:2017 Energy performance of buildings - Method for calculation of system energy requirements and system efficiencies - Part 4-5: District heating and cooling
• Directive (EU) 2018/2001 on the promotion of the use of energy from renewable sources, 2018-12-11. Annex V, C. Methodology, b) and Annex VI, B. Methodology, d)