It is convenient to define an eddy of wave number κ as a disturbance containing energy between 0.62 and 1.62 . This choice centers the energy around a logarithmic scale, since ln (1.62) ln (1/0.62) 1/2. It also makes the width of the contribution to the spectrum equal to (see Fig. 24.1). The eddy size l is roughly equal to 2π/ . This schematic eddy will be used to answer the questions raised earlier.
The energy of an eddy of size 2π/ is roughly proportional to E( ) times the width of the spectrum, . Thus we can identify a characteristic velocity of this eddy as { E( )} 1/2 . Thus the characteristic strain rate of an eddy of wave number κ is
in the central part of the spectrum. Thus
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(24.1) |
Thus the strain rate increases with . Note as increases the eddy size decreases. In other words the strain rate increases as eddy size decreases.
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