Figure 1: A Fractal in the Phase Diagram for One Specification of Parameters in the Kaldor Model^{1} |

**1.0 Introduction**

I thought I would try to combine an ability for computers to draw fractals with an economic model that suggests practical conclusions. In this post, I merely duplicate some results in the literature. In a deterministic ergodic process, as I understand it, all trajectories pass through every state in whatever attractor may exist. Hence, the Kaldor model, like some dynamical systems arising in mathematics, is non-ergodic.

**2.0 The Model**

In 1940, Nicholas Kaldor proposed a model of the business cycle.
It can be expressed by four equations^{2}.
National ouput evolves from the previous period as a response to
aggregate demand:

whereY_{t+1}=Y_{t}+α(I_{t}-S_{t}),

*Y*

_{t}is the value of output in year

*t*,

*I*

_{t}is intended investment, and

*S*

_{t}is intended saving. The parameter

*α*represents the speed of adjustment to excess aggregate demand. The evolution of the value of the capital stock depends on investment and depreciation:

whereK_{t+1}=I_{t}+ (1 -δ)K_{t},

*δ*is the depreciation rate of capital stock. Intended saving is directly proportional to output:

whereS_{t}=σY_{t},

*σ*is the (average and marginal) propensity to save. An investment function

^{3}is the final equation specifying the model:

whereI_{t}=σμ+γ(σμ/δ-K_{t}) + Tan^{-1}(Y_{t}-μ),

*μ*is the expected level of output, and

*γ*represents the costs of adjusting the capital stock. Along with some restrictions on the values of parameters, the model is now fully specified. The arc tangent function provides a s-shaped non-linear term, such that entrepreneurs increase investment when output exceeds their expectations

^{4}.

I find it convenient to define new variables normalized around a stationary state:

k_{t}=K_{t}-σμ/δ

The model, expressed in terms of normalized capital stocks and normalized output, is:y_{t}=Y_{t}-μ

k_{t + 1}= Tan^{-1}(y_{t}) + (1 -δ-γ)k_{t}

Note that the following is a solution:y_{t + 1}= (1 -ασ)y_{t}+αTan^{-1}(y_{t}) -αγk_{t}

For all timet,y_{t}=k_{t}= 0.

**3.0 Some Results**

The above version of the Kaldor model is a discrete-time dynamical system, defined by a map from the two-dimensional real plane (*k*, *y*) to the same space. Four^{5} parameters are used to define the map. Questions for the mathematician revolve around describing how the phase portrait for the system varies qualitatively with variations in the parameters. Complex and chaotic behavior can arise in the Kaldor model with appropriate choices of parameter values.

For a small enough speed of adjustment and large enough propensity to save, the dynamics is boring. All trajectories converge to the origin.

As the propensity to save decreases, the system goes through a pitchfork bifurcation, so-called because the bifurcation diagram looks like a pitchfork. The origin loses its stability, and two symmetric fixed points appear. For a small enough speed of adjustment, at least, the two symmetric fixed points exhibit local asymptotic stability. The location of these new fixed points must be found numerically. A fortiori, the computer must be used as an aid to perform a local stability analysis of these points, based on the eigenvalues of the Jacobian matrix.

As the speed of adjustment increases, the boundary between the basins of attraction becomes more complex. Figure 1 shows a case where they are entangled in a fractal-like structure, and the outer perimeter of the colored area is repelling. The limit cycle shown is a short distance outside this repelling boundary.

I have by no means exhausted the dynamics of the Kaldor model. Consider a region in which the origin is the only fixed point, and it is asymptotically stable. As the speed of adjustment increases, the system undergoes a Neimark-Sacker bifurcation, which, I gather, is the discrete-time analog to a Hopf bifurcation. Cycles exist in which the cycle is not a fixed point on the Poincaré return map, but winds around many times before repeating. And if I want my application to explore all these dynamics, I have quite a bit of programming to do. I am curious if I will be able to plot a bifurcation diagram, given that the behavior at the limit depends on the initial value.

**4.0 Observations**

For the parameter values illustrated in the figures, trajectories have three possible destinations:

- A stable equilibrium with lots of capital and high output.
- Another stable equilibrium with less capital and less output.
- A business cycle.

Although not illustrated above, the model exhibits structural instability. A perturbation of the model parameters can result in different observable behavior, of greater or less complexity.

One general way of conceptualizing business cycles is to see them as the response of a damped linear system to exogenous shocks. Their height and depth depends on the characteristics of the external impulses driving the system. The Kaldor model suggests another possibility. In this model, the properties and extent of business cycles are endogenously determined. Shocks can drive the system from one trajectory to another, but the range of possible behaviors is determined from within the system. It is my impression that the former way of understanding business cycles is dominant among mainstream macroeconomists, while the latter is closer to describing actually existing capitalist economies.

**Footnotes**

- Figure 1 is drawn with the parameter values specified in Figure 2(c) in Agliari et al (2007).
- Kaldor uses a nonlinear savings function and merely specifies the form of the investment function.
- The specification of investment independent of saving is an essential characteristic of Keynesian models.
- In this model, expectations are held constant.
- Notice the expected level of output does not appear in the two equations giving the normalized model.

**Selected References**

- A. Agliari, R. Dieci, and L. Gardini (2007). Homoclinic Tangles in a Kaldor-like Business Cycle Model.
*Journal of Economic Behavior & Organization*. Vol. 62: 324-347. - W. W. Chang and D. J. Smyth (1971). The Existence and Persistence of Cycles in a Non-linear Model: Kaldor's 1940 Model Rexamined.
*Review of Economic Studies*. Vol. 38, No. 1: 37-44. - Richard M. Goodwin (1951). The Nonlinear Accelerator and the Persistence of Business Cycles.
*Econometrica*. Vol. 19, No. 1: 1-17. - Nicholas Kaldor (1940). A Model of the Trade Cycle.
*Economic Journal*. Vol. 50, No. 197: 78-92. - Yuri A. Kuznetsov (1998).
*Elements of Applied Bifurcation Theory*, 2nd edition.

## 11 comments:

Hmm, this looks more like the mathematical masturbation one associates with the modern neoclassical DSGE crowd. Its useless for understanding reality.

What about some real thinking, like Minsky and Keynes showed us ?

Anon,

I don't want to sound like a mainstream economist but you *possibly* sound like you simply didn't understand or couldn't be bothered to understand the maths here, and your comment is borne more of a knee-jerk reaction to maths in economics than healthy pessimism.

No, anon, it doesn't look anything like the models you describe. Indeed, if the four relations in the model were described, it would be readily understood to be very closely related to General Theory thinking.

This type of mathematical exploration does not

derivethe relationships from armchair theorizing that all people in society make all decisions according to some 19th century long-since falsified stereotype ~ rather, it explores how the system would work depending on how strongly or weakly and how rapidly or slowly the relationships in the model work.From this, unlike the a priori mainstream modeling based on known false assumptions, one can indeed pursue actual scientific exploration to determine whether significant relations have been omitted, and for the relations in the model how strong and rapid the relations appear to be.

Its no accident that when Steve Keen pursues his research on Minsky's theory, he relies heavily on computer modeling of dynamic relations.

I thought this was a great post. I teach the chalk board version of the model but have never thought it through to a model of the business cycle.

Should have read "endogenous model" of the BC

How do you make these non-ergodic models? Which program do you use to draw the solutions? I think this kind of approach may help to design growth models including business cycles, and forget narrow-minded "stable" or "explosive" models towards a more complex way of thinking.

Genaro, I have been writing my own Java programs. I do not have a general program for exploring dynamical systems. Rather, I have been writing custom programs. You probably can do something like this in Matlab, Octave, or Mathematica. Part of the point for me is to review Java.

In the General Theory, Keynes assumes that short run expectations, on the level of capacity utilization, are usually adjusted until they are met. But long run expectations, on the amount of capacity, are given. When long run expectations can be compared with results, it is too late to do anything about their failure. So, to expand on Bruce's point, Kaldor's assumption of a given expectation for income and the corresponding needed capital is an extremely simple way of building on Keynes, in my opinion. (I have previously mentioned extending Keynes to the long period. Debates have arisen in the literature on whether these extension treat finance at all adequately.)

http://nakedkeynesianism.blogspot.com.ar/2012/03/sraffian-economics-vs-post-keynesian.html#comment-form

Here's an interesting explanation for growth theories from Vernengo. I think Kaldor's model does not fit in (C). Kaldor model implies that, when capitalists decide to invest, they don't ever think they won't sell the production. Expected demand has to be pro-cycle at least. They cannot be fixed, they have to tend towards a capital accumulation path. This does not mean that there is a long term equilibrium or full utilisation of resources, because the model tends to a normal utilisation level, and "equilibrium" relies on the exogenous demand growth rate, wich is always changing.

The normal accumulation path is the fixed point (k, y) = (0, 0). This fixed point is different than the other two. Expectations are not being met at the other two points.

I don't think one should require that the normal accumulation path be stable. The sun works as a center of gravitational attraction, even if the earth will never crash into it.

More seriously, to see models of complex dynamics in which cycles and growth paths cannot be analyzed separately, see the work of Richard Goodwin.

Steve Keen is also an excellent source to look for.

http://www.debtdeflation.com/blogs/qed/

I recommend his lectures as well!

Greetings

Georg

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