In the following problems, ideal op-amps are assumed. This op-amp circuit appears in Dorf's Modern Control Systems, 12th Edition (pg. 136):
With \$v_{in}\$ on the left and \$v_{o}\$ on the right. Dorf's answer key gives
$$ \frac{v_{o}}{v_{in}} = 1 + \frac{R_{2}}{R_{1}}. $$
How? A different problem gives a similar answer:
Where the answer is derived as follows:
$$ v_{o} = A(v_{+} - v_{-}) $$ $$ v_{o} = A(v_{in} - v_{o}\frac{R_2}{R_2 + R_1}) $$ $$ v_{o} = \frac{Av_{in}}{1 + A\frac{R_2}{R_2 + R_1}} $$ $$ \frac{v_{o}}{v_{in}} = \frac{R_2+R_1}{R_2} $$ $$ \frac{v_{o}}{v_{in}} = 1+\frac{R_1}{R_2} $$
because \$A>>1\$.
I don't see how the first circuit yields an answer so similar to the second when its configuration is apparently different.
I'm not even sure how to go about solving circuit one; normally I'd use KCL on the \$v_o\$ node but there's no current through \$R_2\$.