Classic differential amplifier. Resistors \$R_F\$ and \$R_A\$ connected to non-inverting and inverting inputs of-amp are the same, respectively, so the simplest way to calculate output voltage shall be:
$$
V_{out} = \frac{R_A}{R_F} \cdot (V_+ - V_-)
$$
$$
V_{out} = \frac{70k\Omega}{0.4k\Omega} \cdot -0.1V = -17.5V
$$
But... there is internal resistance of voltage source \$R_i\$ which is in series with resistor \$R_F\$ connected to non-inverting input, so we need to use a full equation for differential amplifier, and assume that \$R_{Fi}\$ is a sum of \$R_F\$ and \$R_i\$:
$$
V_{out} = \frac{(R_A + R_{Fi})R_A}{(R_A + R_F)R_{Fi}} \cdot V_+ - \frac{R_A}{R_{Fi}} \cdot V_-
$$
In above equation \$V_+\$ and \$V_-\$ are potentials referenced to ground. To obtain theme You should remember that both inputs of an op-amp are considered to be on ground level all the time. So \$E\$, its internal resistance and \$R_F\$ resistors create simple circuit with common current flowing through them. This current is:
$$
I_E = E / (R_i + R_F + R_F) = 0.1V / (0.14 + 0.4 + 0.4)k\Omega \approx 106.4{\mu}A
$$
Voltage drop at \$R_F\$ is:
$$
V_{R_F} = I_E \cdot R_F = 106.4{\mu}A \cdot 0.4k\Omega = 42.5mV
$$
So potential \$V_+\$ (connection point of lower \$R_F\$ and \$E\$) is \$-42.5mV\$, referenced to ground. And potential \$V_-\$ (connection point \$R_i\$ and \$E\$) is \$57.5mV\$, \$100mV\$ higher than \$V_+\$.
Now, we know everything:
$$
V_{out} = \frac{(70k\Omega + 0.54k\Omega)70k\Omega}{(70k\Omega + 0.4k\Omega)0.54k\Omega} \cdot -42.5mV - \frac{70k\Omega}{0.54k\Omega} \cdot 57.5mV \approx -12.97V
$$
Current flows through the \$R_A\$ is:
$$
I_A = V_{out} / R_A = -12.97V / 70k\Omega \approx 185.3{\mu}A
$$
As user1521378 suggest You can also assume that \$V_-\$ will be at connection point of upper \$R_F\$ and internal resistance of \$E\$, then You should calculate potential at this point in the same manner like for \$V_+\$ and use first simple equation to obtain output voltage.