Note that there is no voltage drop across the ammeter. Thus, the currents in the bottom resistors are the same, which we call i (so the current through the battery is 2i and the voltage drop across each of the bottom resistors is iR ). The resistor network can be reduced to an equivalence of
Req=(2R)(R)2R+R+(R)(R)R+R=76R
which means that we can determine the current through the battery (and also through each of the bottom resistors):
2i=εReq⇒i=ε2Rq=ε2(7R/6)=3ε7R
By the loop rule (going around the left loop, which includes the battery, resistor 2R, and one of the bottom resistors), we have
ε−i2R(2R)−iR=0⇒i2R=ε−iR2R
Substituting i=3ε/7R, this gives i2R=2ε/7R. The difference between i2R and i is the current through the ammeter. Thus,
iammeter =i−i2R=3ε7R−2ε7R=ε7R⇒iammeterε/R=17=0.143