Scientific American Supplement, No. 787, January 31, 1891 eBook

This eBook from the Gutenberg Project consists of approximately 142 pages of information about Scientific American Supplement, No. 787, January 31, 1891.

Scientific American Supplement, No. 787, January 31, 1891 eBook

This eBook from the Gutenberg Project consists of approximately 142 pages of information about Scientific American Supplement, No. 787, January 31, 1891.

BATTERY GROUPING FOR QUICKEST ACTION.

One may consider the question of grouping the battery cells from the same point of view.  How does the need for rapid working, and the question of time constant, affect the best mode of grouping the battery cells?  The amateur’s rule, which tells you to so arrange your battery that its internal resistance should be equal to the external resistance, gives you a result wholly wrong for rapid working.  The supposed best arrangement will not give you (at the expense even of economy) the best result that might be got out of the given number of cells.  Let us take an example and calculate it out, and place the results graphically before our eyes in the form of curves.  Suppose the line and electromagnet have together a resistance of 6 ohms, and that we have 24 small Daniell cells, each of electromotive force say 1 volt, and of internal resistance 4 ohms.  Also let the coefficient of self-induction of the electromagnet and circuit be 6 quadrants.  When all the cells are in series, the resistance of the battery will be 96 ohms, the total resistance of the circuit 102 ohms, and the full value of the current 0.235 ampere.  When all the cells are in parallel, the resistance of the battery will be 0.133 ohm, the total resistance 6.133 ohms, and the full value of the current 0.162 ampere.  According to the amateur rule of grouping cells so that internal resistance equals external, we must arrange the cells in 4 parallels, each having 6 cells in series, so that the internal resistance of the battery will be 6 ohms, total resistance of circuit 12 ohms, full value of current 0.5 ampere.  Now the corresponding time constants of the circuit in the three cases (calculated by dividing the coefficient of self-induction by the total resistance) will be respectively—­in series, 0.06 sec.; in parallel, 0.5 sec.; grouped for maximum steady current, 0.96 sec.  From these data we may now draw the three curves, as in Fig. 55, wherein the abscissae are the values of time in seconds and the ordinates the current.  The faint vertical dotted lines mark the time constants in the three cases.  It will be seen that when rapid working is required the magnetizing current will rise, during short intervals of time, more rapidly if all the cells are put in series than it will do if the cells are grouped according to the amateur rule.

|
5|                                                           .
|                                                      .
|                                                 .
4|                           MAXIMUM         .
|                          OUTPUT \    .
|                                 .
3|                             .
|                          .  :      ALL IN SERIES
|         _-------------------:------------------------------
2|      .-             —       : 
|    -            -           : 
|  -:          -               : 
1| / :       —                  :              ALL IN PARALLEL
|.  :   .                      :              _________--------
|-  :__      :       ----------
+-----------------------------:-------------------------------
0     1     2     3     4     5     6     7     8     9    10

FIG. 55.—­CURVES OF RISE OF CURRENT WITH DIFFERENT GROUPINGS OF BATTERY.

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Scientific American Supplement, No. 787, January 31, 1891 from Project Gutenberg. Public domain.