The solution of nonlinear inverse problems and the Levenberg-Marquardt method

Geophysics ◽  
2007 ◽  
Vol 72 (4) ◽  
pp. W1-W16 ◽  
Author(s):  
Jose Pujol

Although the Levenberg-Marquardt damped least-squares method is an extremely powerful tool for the iterative solution of nonlinear problems, its theoretical basis has not been described adequately in the literature. This is unfortunate, because Levenberg and Marquardt approached the solution of nonlinear problems in different ways and presented results that go far beyond the simple equation that characterizes the method. The idea of damping the solution was introduced by Levenberg, who also showed that it is possible to do that while at the same time reducing the value of a function that must be minimized iteratively. This result is not obvious, although it is taken for granted. Moreover, Levenberg derived a solution more general than the one currently used. Marquardt started with the current equation and showed that it interpolates between the ordinary least-squares-method and the steepest-descent method. In this tutorial, the two papers are combined into a unified presentation, which will help the reader gain a better understanding of what happens when solving nonlinear problems. Because the damped least-squares and steepest-descent methods are intimately related, the latter is also discussed, in particular in its relation to the gradient. When the inversion parameters have the same dimensions (and units), the direction of steepest descent is equal to the direction of minus the gradient. In other cases, it is necessary to introduce a metric (i.e., a definition of distance) in the parameter space to establish a relation between the two directions. Although neither Levenberg nor Marquardt discussed these matters, their results imply the introduction of a metric. Some of the concepts presented here are illustrated with the inversion of synthetic gravity data corresponding to a buried sphere of unknown radius and depth. Finally, the work done by early researchers that rediscovered the damped least-squares method is put into a historical context.

2015 ◽  
Vol 2015 (1) ◽  
Author(s):  
Abdul Latif ◽  
Abdulaziz SM Alofi ◽  
Abdullah E Al-Mazrooei ◽  
Jen-Chih Yao

Geophysics ◽  
1969 ◽  
Vol 34 (1) ◽  
pp. 65-74 ◽  
Author(s):  
William W. Johnson

The equations relating the magnetic anomalies to the shape and susceptibility of a body are nonlinear with respect to the coordinates describing the shape. Therefore, iterative procedures must be used to obtain least‐squares estimates of the body coordinates. One method in general use for obtaining nonlinear least‐squares estimates is the Gauss method. This method often fails when the initial values for the structures and susceptibilities do not adequately account for the magnetic anomalies. Another method known as the steepest descent method generally converges to a solution; however, a large number of iterations are required. A method suggested by Marquardt (1963) incorporates the best features of the previous methods. In this paper the Marquardt method is applied to the interpretation of magnetic anomalies. For this purpose the two‐dimensional formulas derived by Talwani and Heirtzler (1964) are used to relate the geometry of a body to the resulting magnetic anomalies. The procedure efficiently controls the amount of change made to an interpreted structure at each iteration, assuring rapid convergence to a solution which satisfies the observed data better in the least‐squares sense than does the initial solution. The method is applied to representative problems.


Geophysics ◽  
1981 ◽  
Vol 46 (12) ◽  
pp. 1745-1748 ◽  
Author(s):  
K. K. Khurana ◽  
S. V. Seshagiri Rao ◽  
P. C. Pal

The elegance and ease with which the Fourier transformation method can be employed in the interpretation of potential field geophysical data (Dean, 1958; Gudmundsson, 1966) has resulted in the formulation of a number of frequency‐domain approaches for interpreting the magnetic effects of specific source geometries, e.g., Bhattacharyya (1966), Sengupta (1974), Sengupta and Das (1975), Bhattacharyya and Leu (1975, 1977), etc. In these techniques, the parameters of interest are estimated from the characteristics of the amplitude and phase spectra, a process that is often beset with several problems which adversely affect the estimation of parameters. These problems arise partly from the ill‐defined nature of characteristic points in the spectra, either due to spectral noise or due to inadequate digitization spacing, and partly from the fact that the errors in the estimation of certain parameters which are used for subsequent estimation of the other parameters usually cause added spectral distortions. Rao et al. (1978) advocated the use of end corrections to overcome these problems. An effective alternative would be to incorporate the least‐squares method in the interpretational process. This necessitates iteration owing to the nonlinear nature of equations relating the source parameters and the Fourier spectra of corresponding anomalies. While it is tempting to employ the iteration scheme formulated by Gauss in 1821 for this purpose, as has indeed been done in a number of space‐domain approaches (e.g., Hall, 1958; Bosum, 1968; Al‐Chalabi, 1970; Rao et al., 1973; Won, 1981), the convergence in this approach requires the initially assumed values of the parameters to be very close to the final solution. The steepest descent method, an alternative to this, has an extremely slow convergence. It is shown here, with the example of a two‐dimensional (2-D) structure, that Marquardt’s algorithm (Marquardt, 1963), which offers a compromise between these two iteration schemes and has been effectively employed by Johnson (1969) and Pedersen (1977) in their space‐domain interpretation schemes, provides an efficient approach to accomplish the iteration in the case of frequency‐domain magnetic interpretation.


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