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  • 1
    Electronic Resource
    Electronic Resource
    Cambridge : Cambridge University Press
    Modern Asian studies 20 (1986), S. 793-820 
    ISSN: 0026-749X
    Source: Cambridge Journals Digital Archives
    Topics: Ethnic Sciences , History , Political Science , Economics
    Notes: Feeling strong pressure from Western Powers Japan abandoned her seclusion policy in 1854 and inaugurated serious efforts to modernize her society and economy after the Meiji Restoration in 1868. She, in turn, forced Korea who had been keeping the seclusion policy on her own to open the door in 1876. The feudal Korean government (the Yi Dynasty, 1392–1910) was impelled to embark on social and economic reforms by opening the door. Yet, after nearly thirty years’ struggle to make reforms and to secure the independence of the country, Korea was converted into a protectorate of Japan in 1905 and was officially annexed to her in 1910. The Japanese government recognized that the creation of modern monetary and banking systems in Korea was the precondition for trade expansion between the two countries (for Japan, rice imports on the one hand and textile exports on the other) and thus started its colonial rule over Korea by establishing a central bank, development banks and financial cooperatives. This paper aims at setting forth an analysis of a more or less unexplored field in the study of the economic history of Korea, that is, the financial aspects of her economic growth under Japanese rule. Particularly, emphasis will be placed on quantitative analysis of major financial variables represented by money, interest rates and bank credit. Before proceeding to the main subject, it may well serve to review some of the financial problems in the late Yi Dynasty period.
    Type of Medium: Electronic Resource
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  • 2
    Publication Date: 1986-05-01
    Description: A pseudo-spectral numerical scheme is used to study two-dimensional, single-cell, time-dependent convection in a square cross-section of fluid saturated porous material heated from below. With increasing Rayleigh number R convection evolves from steady S to chaotic NP through the sequence of bifurcations S→ P(1) → QP2→ p(2) → NP, where P(1) and P(2) are simply periodic regimes and QP2 is a quasi-periodic state with two basic frequencies. The transitions (from onset of convection to chaos) occur at Rayleigh numbers of 4π2380–400, 500–520, 560–570, and 850–1000. In the first simply periodic regime the fundamental frequency f1 varies as R7/8and the average Nusselt number Nu is proportional to R2/3; in P(2)f1varies as R3/2 and Nu oc R11/10. Convection in QP2 exhibits hysteresis, i.e. if the QP2 state is reached from P(1)(P(2)) by increasing (decreasing) R then the frequency with the largest spectral power is the one consistent with the extrapolation of f1 according to R7/8(R3/2). The chaotic states are characterized by spectral peaks with at least 3 fundamental frequencies superimposed on a broadband background noise. The time dependence of these states arises from the random generation of tongue-like disturbances within the horizontal thermal boundary layers. Transition to the chaotic regime is accompanied by the growth of spectral components that destroy the centre-symmetry of convection in the other states. Over-truncation can lead to spurious transitions and bifurcation sequences; in general it produces overly complex flows. © 1986, Cambridge University Press. All rights reserved.
    Print ISSN: 0022-1120
    Electronic ISSN: 1469-7645
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
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