Full text: Allgemeine Theorie des Electrodynamometers

$ 56. INTEGRATION DER DIFFERENTIALGLEICHUNGEN DER ZWEITEN ANNÄHERUNG. 69 
  
  
  
Ey Y e-kıt 5 ge Mt rg at Met petit 
e kat 12, — 2) letrtdt= = a ET +rate”". on en th a NG a 
Fe (kg 2 0 (ky +2c)t NEL (kg+2c)t . Te ct ı Da a 
ı aoı..ıx x ot "io -ı  — 
rise Act flo Pre 2ct Fer Y en 
a een r u un 
Man setze nun hier zur Abkürzung die constanten Coöfficienten der gesuchten Differenz : 
a a ro 
u 
  
  
  
  
  
  
  
  
  
  
  
  
  
  
Ir Depp 
I m —_ z = 
k—kı ok, (ko—k)? 
Try Keen 
0 Do ne 
LI 0 nn 
RER | RR EEE 
a 0 u 
OR 
E 1 
ei 
o—kı ı—2kg % ( Er —k,) 
ae et Vo 
“u. a. 5 a kg) © 
lt a  £ 
2 o—kı | kn —ko—t “ n = ko—kıte) ni 
nn a 1 an Ng = 
ee ne S on S on 
u. —kı Y\ kg —% 7% | as ae: 8 
ca To 1 a 1 Bi Tr f 1 as 1 = Yıo ar kıtka—2c = 
Ta hin cum kl (ko)? (ka—e)? (ee ee 
a u 1 = 1 5 f 1 1 = Fa EN k, ko alle z 
UT lu ok | al) 5 
a Alk, 20): le 20) 
1 I Tjg 
er eerresseniarmwennmer 
k 
Tja 1 1 - an 
| 
  
  
nn 5. (kA) (ko—Ac) n 
1 = 1 = Ya ” 
HM u er m dd 
— "5 (8 eh 1 = a, 
_ Ka) 2) ° 
  
  
  
5, (ge—k,)= ke = —$,(kg—k}) 
  
+5,(ka—k)= SER ae — +35, (ko—kı). 
 
	        
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