The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1925 - Physics |
From inside the book
Results 1-5 of 95
Page 1
... error permissible , ( 3 ) the natural frequency and damping of the instrument . When the oscil- lograph ( which ... errors of 0.7 per cent . and 40 per.
... error permissible , ( 3 ) the natural frequency and damping of the instrument . When the oscil- lograph ( which ... errors of 0.7 per cent . and 40 per.
Page 2
... errors not exceeding 0.7 per cent . , and from 0 to 0-2n for a 40 per cent . error . With certain curves , however ( i . e . pure sine waves with or without slight damping ) , the error is of no account , provided that the amplitude ...
... errors not exceeding 0.7 per cent . , and from 0 to 0-2n for a 40 per cent . error . With certain curves , however ( i . e . pure sine waves with or without slight damping ) , the error is of no account , provided that the amplitude ...
Page 9
... Error At p = 0 Ā· 2n R 1 L = k and LC = n2 . Fig . 3 . ( C ) 4 % Error ! At p = n 80 ( a ) 70 60 50 ( c ) .. ( a ) Uncompensated Curve ( K = 2n ) . ( b ) Compensated Curve ( Range increased 5 times ) . " " With same zero . Amplitude as ...
... Error At p = 0 Ā· 2n R 1 L = k and LC = n2 . Fig . 3 . ( C ) 4 % Error ! At p = n 80 ( a ) 70 60 50 ( c ) .. ( a ) Uncompensated Curve ( K = 2n ) . ( b ) Compensated Curve ( Range increased 5 times ) . " " With same zero . Amplitude as ...
Page 10
... error , for example , would be involved within the range p = 0 to p = 0 Ā· 2n for curve ( a ) , while the range in which the same error would be incurred in curves ( b ) and ( c ) is from 0 to n , or from 0 to 0.2N . The working range ...
... error , for example , would be involved within the range p = 0 to p = 0 Ā· 2n for curve ( a ) , while the range in which the same error would be incurred in curves ( b ) and ( c ) is from 0 to n , or from 0 to 0.2N . The working range ...
Page 14
... error . When a suitable position for the magnet had been found , it was left set in that position during the whole of the subsequent experiments . The natural frequency of vibration of the reed must be known . This was ascertained in ...
... error . When a suitable position for the magnet had been found , it was left set in that position during the whole of the subsequent experiments . The natural frequency of vibration of the reed must be known . This was ascertained in ...
Contents
17 | |
27 | |
60 | |
61 | |
71 | |
86 | |
97 | |
112 | |
389 | |
399 | |
409 | |
423 | |
439 | |
453 | |
463 | |
470 | |
113 | |
141 | |
157 | |
173 | |
180 | |
187 | |
195 | |
205 | |
226 | |
250 | |
263 | |
289 | |
306 | |
341 | |
345 | |
360 | |
375 | |
381 | |
471 | |
491 | |
504 | |
505 | |
512 | |
521 | |
536 | |
547 | |
553 | |
570 | |
589 | |
600 | |
612 | |
618 | |
624 | |
637 | |
645 | |
663 | |
Other editions - View all
Common terms and phrases
absorption aluminium amalgam amplitude angle apparatus approximately atoms B-rays bands bismuth bubble calculated cent chamber charge coefficient column constant corresponding crystal curve deflexion determined diameter displacement effect electric electrolyte electrons emission energy equation error experimental experiments filament formula frequency galvanometer gases give given grid heat helium hydrogen increase inductance intensity investigation ionization ionization chamber ionization gauge ionization potential lines liquid magnetic field maximum measured mercury metals method molecules motion negative negative bands observed obtained orbits oscillograph oxide paper particles Phil photoelectric effect photograms Phys pipe plate positive potassium potential pressure Proc quantum radiation radius ratio resistance change shows sinĀ² single scattering solution spectra spectrum structure surface combustion Table temperature terminal velocity theoretical theory tube values vapour vibrations viscosity voltage volts wave-length X-ray zero