The right answer is 5V as the others already explained. I'll assume you have a sinusoidal signal applied (otherwise you would have got a different result).
Impedance of the resistor is \$R\$, which is a real value.
Impedance of the inductor is \$j\omega L\$, which is complex. While multiplying by a real value scales a vector, multiplying by (a power of) \$j\$ rotates it in the complex plane. Multiplying by \$j\$ gives a 90° rotation, \$ \times j^3\$ is 3 \$\times\$ 90°, and \$ \times \sqrt{j}\$ will give a 45° rotation, for instance.

(In the image \$i\$ is used instead of \$j\$. That's what mathematicians use. In electronics \$j\$ was chosen because \$i\$ was already used to indicate current.)
\$V_R = I \times R\$
Voltage and current have the same phase; their vectors point in the same direction.
\$V_L = I \times j\omega L \$
The factor \$j\$ causes a 90° rotation of the \$I\$ vector, so the voltage is at a right angle.
Now \$I\$ is the same for resistor and inductor since they're in series. \$V_R\$ is in phase with \$I\$, and \$V_L\$ is at 90° with that same \$I\$, therefore \$V_L\$ and \$V_R\$ are at a right angle. Adding them gives you a right-angle triangle, and you can apply Pythagoras to find the magnitude of the sum:
\$ |V| = \sqrt{|V_L|^2 +|V_R|^2} = \sqrt{(3V)^2 +(4V)^2} = 5V \$
The phase difference between current and voltage is
\$ \phi = arctan\left(\dfrac{V_L}{V_R}\right) = arctan\left(\dfrac{3V}{4V}\right) = 37°\$