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It is shown that, when the mass of an elastc body of linear form is supported to be condensed into rigid masses to particles situated at the mid-points of equal segments while the elastic properties of the body are unaltered, the error in the frequency of any natural mode of oscillation ultimately varies inversely as the square of the number of segments. When the mass are not placed at the midpoints of the segments the error varies ultimately as the inverse first power of the number of segments. The general conclusions are checked by numerical examples and by comparison with cases where exact solutions for the semented bodies are available.
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W.J. Duncan (1952) studied this question.
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