How are complex number being treated in physics? In various places in physics, EM for example, complex numbers are used to describe things that are physically real. I will point a simple case - solving an ODE for resistance/charge/voltage. We get a certain value, which is in the form $a+bi$ and take its real part. My question is, what does the imaginary part of the answer physically represents? How do we know we are not "losing information" by considering only the real part when using complex numbers in calculations? The whole treatment of complex numbers in physics baffles me. What does the complex plane have to do with reality? Sometimes certain motions are also described with complex numbers.
 A: The question is based on a false premise:  that only the real part of complex current or voltage is significant.
In fact, it is the magnitude of the complex quantity that is significant.  The relationship between the real and imaginary parts tells you the timing or phase of the quantity relative to a pure resistance
If you had a circuit with a resistor, capacitor and inductance arranged in series and fed with $120$ V alternating current, you could calculate that the voltage across the inductance and the capacitor were both purely imaginary. Yet a AC voltmeter could measure a very real voltage across each of these.  More importantly, you could get blown on your backside by this imaginary voltage, if you were to touch the capacitor or inductance at the wrong moment in the alternating voltage.
As a different example: If you were to calculate the voltage individually across four circuit elements in series and find $$V_1=(5+0i) \text{ Volts}$$$$V_2=(0+5i) \text{ Volts}$$$$V_3=(0-5i) \text{ Volts}$$$$V_4=(3+4i) \text{ Volts}$$then you would know that the measured voltage across each of the elements would be exactly the same, $5$ Volts.
If you were to display the voltages on a multiple trace oscilloscope, you would see four identical sine waves with an amplitude of $5$ Volts: $V_2$ would be $90$ degrees out of phase with $V_1$, $V_3$ would be $180$ degrees out of phase with $V_2$, and $V_4$ would be $53.13$ degrees out of phase with $V_1$ $( \text{ because }\tan(53.13)=\frac{4}{3})$
A: In the simplest case we may use an exponential like an $A\cdot \text{e}^{\text{i}\omega t}$ instead of a $A\cdot\sin(\omega t)$, so it is just the easiest way of writing the solutions (simplest harmonic oscillations).
But in reality the amplitude and the phase may vary with time in the transient processes, so you must write two equations instead of one. Often these two equations are equivalent to one equation with a complex coefficients and solutions simply connected to the variables in question.
A: Certainly you lose information by only taking the real part of a complex number, but sometimes that is the only part you are interested in. In the case of resistance, the complex quantity is called impedance, and the imaginary part (called reactance) covers the effect of capacitors and inductances.
In general complex numbers are used because they make the Maths easier. An unexpected complex answer, like getting $sin\theta>1$ in Snell's Law, tells you something different is happening.
A: another example:
to solution of this  differential equation:
$${\frac {d^{2}}{d{t}^{2}}}x \left( t \right) +{\omega}^{2}x \left( t
 \right) +2\,\gamma\,{\frac {d}{dt}}x \left( t \right)=0
$$
is: (Ansatz)
$$x(t)= \left( a+ib \right) {{\rm e}^{ \left( -\gamma+i\sqrt {-{\gamma}^{2}+{
\omega}^{2}} \right) t}}+ \left( a-ib \right) {{\rm e}^{ \left( -
\gamma-i\sqrt {-{\gamma}^{2}+{\omega}^{2}} \right) t}}
$$
where the imaginary part of x(t) is zero .
Thus : because  $\Im(x(t))=0$ , the solution is  $\Re(x(t))$
with the   initial condition
$$x(0)=x_0\quad ,\dot{x}(0)=v_0$$
you have two equations for $a$ and $b$
$$a=\frac{x_0}{2}$$
$$b=\frac{1}{2}\,{\frac {x_{{0}}\gamma+v_{{0}}}{\sqrt {-{\gamma}^{2}+{\omega}^{2}}}}$$
