Lumped-element model: Difference between revisions

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{{short description|Simplification of a physical system into a network of discrete components}}
{{Technical|date=August 2019}}
{{Refimprove|date=August 2023}}
[[File:Ohm's Law with Voltage source TeX.svg|thumb|Representation of a lumped model made upconsisting of a voltage source and a resistor.]]
 
The '''lumped-element model''' (also called '''lumped-parameter model''', or '''lumped-component model''') simplifiesis thea description[[idealization (philosophy of thescience)|simplified]] behaviourrepresentation of spatially distributeda [[physical systems,system]] suchor ascircuit electricalthat circuits,assumes intoall components are concentrated at a [[Topologysingle (electricalpoint circuits)|topology]]and consistingtheir ofbehavior discretecan entitiesbe thatdescribed approximateby theidealized behaviourmathematical ofmodels. theThe distributedlumped-element model simplifies the system underor certaincircuit assumptionsbehavior description into a [[Topology (electrical circuits)|topology]]. It is useful in [[electrical network|electrical systems]] (including [[electronics]]), mechanical [[multibody system]]s, [[heat transfer]], [[acoustics]], etc. This mayis bein contrastedcontrast to [[distributed parameter system]]s or models in which the behaviour is distributed spatially and cannot be considered as localized into discrete entities.
 
Mathematically speaking, theThe simplification reduces the [[State space (controls)|state space]] of the system to a [[counting number|finite]] [[dimension]], and the [[partial differential equation]]s (PDEs) of the continuous (infinite-dimensional) time and space model of the physical system into [[ordinary differential equation]]s (ODEs) with a finite number of parameters.
 
== Electrical systems ==
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=== Lumped-matter discipline ===
The '''lumped-matter discipline''' is a set of imposed assumptions in [[electrical engineering]] that provides the foundation for '''lumped-circuit abstraction''' used in [[Network analysis (electrical circuits)|network analysis]].<ref>Anant Agarwal and Jeffrey Lang, course materials for 6.002 Circuits and Electronics, Spring 2007. MIT OpenCourseWare ([http://ocw.mit.edu/courses/electrical-engineering-and-computer-science/6-002-circuits-and-electronics-spring-2007/video-lectures/6002_l1.pdf PDF]), [[Massachusetts Institute of Technology]].</ref> The self-imposed constraints are:
# The change of the magnetic flux in time outside a conductor is zero. <math display="block">\frac{\partial \phi_BPhi_B} {\partial t} = 0</math>
# The change of the charge in time inside conducting elements is zero. <math display="block">\frac{\partial q} {\partial t} = 0</math>
# Signal timescales of interest are much larger than [[propagation delay]] of [[electromagnetic waves]] across the lumped element.
 
The first two assumptions result in [[Kirchhoff's circuit laws]] when applied to [[Maxwell's equations]] and are only applicable when the circuit is in [[steady state (electronics)|steady state]]. The third assumption is the basis of the lumped-element model used in [[Network analysis (electrical circuits)|network analysis]]. Less severe assumptions result in the [[distributed-element model]], while still not requiring the direct application of the full Maxwell equations.
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{{Main|Newton's law of cooling}}
 
'''Newton's law of cooling''' is an [[empirical relationship]] attributed to English physicist [[Isaac Newton|Sir Isaac Newton]] (1642–1727). This law stated in non-mathematical form is the following:
 
{{Quotation|The rate of heat loss of a body is proportional to the temperature difference between the body and its surroundings.}}
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A simplifying assumption in this ___domain is that all heat transfer mechanisms are linear, implying that radiation and convection are linearised for each problem.
 
Several publications can be found that describe how to generate lumped-element models of buildings. In most cases, the building is considered a single thermal zone and in this case, turning multi-layered walls into lumped elements can be one of the most complicated tasks in the creation of the model. The dominant-layer method is one simple and reasonably accurate method.<ref>Ramallo-González, A.P., Eames, M.E. & Coley, D.A., 2013. Lumped Parameter Models for Building Thermal Modelling: An Analytic approach to simplifying complex multi-layered constructions. Energy and Buildings, 60, pp.174-184.</ref> In this method, one of the layers is selected as the dominant layer in the whole construction, this layer is chosen considering the most relevant frequencies of the problem. In his thesis,<ref>Ramallo-González, A.P. 2013. Modelling Simulation and Optimisation of Low-energy Buildings. PhD. University of Exeter.</ref>
 
Lumped-element models of buildings have also been used to evaluate the efficiency of domestic energy systems, by running many simulations under different future weather scenarios.<ref>Cooper, S.J.G., Hammond, G.P., McManus, M.C., Ramallo-Gonzlez, A. & Rogers, J.G., 2014. Effect of operating conditions on performance of domestic heating systems with heat pumps and fuel cell micro-cogeneration. Energy and Buildings, 70, pp.52-60.</ref>
 
== Fluid systems ==
Lumped-elementFluid modelssystems can be useddescribed toby describemeans fluidof systems[[Lumped parameter cardiovascular model|lumped-element cardiovascular models]] by using voltage to represent pressure and current to represent flow; identical equations from the electrical circuit representation are valid after substituting these two variables. Such applications can, for example, study the response of the human cardiovascular system to [[ventricular assist device]] implantation.<ref>Farahmand M, Kavarana MN, Trusty PM, Kung EO. "Target Flow-Pressure Operating Range for Designing a Failing Fontan Cavopulmonary Support Device" IEEE Transactions on Biomedical Engineering. DOI: 10.1109/TBME.2020.2974098 (2020)</ref>
 
== See also ==