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(R, +R,) I)<br />

1(1) = 10 exp( L<br />

(c) Using your results from (b), find the value of the total emf around the circuit (which<br />

from Faraday's law is -Ldl / dl) just after the switch is opened. Is your assumption in (b)<br />

that Go could be ignored for times just after the switch is opened OK?<br />

dIU)1<br />

G=-L--<br />

dt ,.0<br />

=Io(R, +R,)<br />

S· mce 10 =­<br />

Go<br />

,<br />

R '<br />

Go (R, )<br />

G= - (R, +R, )= 1+- Go »Go<br />

R, R,<br />

(": R, »R,)<br />

Thus, the assumption that Go could be ignored for times just after the switch is open is<br />

OK.<br />

(d) What is the magnitude of the potential drop across the resistor R, at times t > 0, just<br />

after the switch is opened? Express your answers in terms of Go , R" and R, . How does<br />

the potential drop across R, just after t = 0 <strong>com</strong>pare to the battery emf Go, if<br />

R, =100R,?<br />

The potential drop across R2 is given by<br />

If R, = 1 OOR"<br />

R, (R, )( R, ) R,<br />

L'>.V, = G= 1 +- Go =-Go<br />

R, + R, R, + R, R, R,<br />

i1V 2 = 100 Eo<br />

This is why you have to open a switch in a circuit with a lot of energy<br />

stored ill the magnetic field very carefully, or you end lip very dead!!

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