As Madmanguruman says, the capacitor is in the wrong place.
The opamp is trying to keep the voltages on it's inverting input the same as the non-inverting input, which is 240mV in your example above. To do this with just Rsense present, it must keep 480mA flowing through Rsense as you say.
Now, with the cap in series, it will actually work to charge the capacitor as you have it. However, the catch is that it will not be at a constant current, and the cap will only charge to 240mV, since this it what the opamp needs to keep the balance.
The cap does not pass DC, so the current is initially 480mA, and drops exponentially down to 0 as the voltage rises (and the voltage across the resistor drops)
Another thing to understand here is that a simulation is only as real as you make it, and in some cases the ideal components cause problems. It's quite common for the simulator not to converge or produce odd results if there is no DC path available. Also with a transient simulation, you sometimes need initial conditions set to observe a process.
For example, if I simulate the above circuit in LTSpice with an ideal 1F capacitor, the simulation does not converge (never finishes) If I add a high value of parallel resistance (10MΩ, this is actually very conservative for such a large value, probably be much lower) to provide a DC path, and (very roughly) simulate real world imperfect capacitor leakage, the simulation works:
Simulation:
The 240mV is produced by the 24nA across the 10MΩ resistance (24e-9 * 10e6 = 0.24V) However, the cap starts the simulation at 240mV. Is this what will happen in real life? It's unlikely, so we need to simulate things as it will be when power is switched on, or at least with the cap starting with 0V across it. The reason this happens (in SPICE at least) is because there is an initial DC operating point simulation done before the transient simulation starts.
If we do the same simulation with an initial condition specified, we can see the "interesting" bit that happens prior to reaching a steady state:
So remember to be aware of the difference between ideal and real world components. If simulation results appear strange, then try adding some ESR/ESL (equivalent series resistance/inductance) and parallel resistances to simulations that correspond with the components you intend to use (datasheet will give values usually)
Also be aware of tolerances, for which monte carlo simulation is very useful.
Finally, here is the circuit with the cap placed in the right place, (although you may want high side current limiting in your final circuit):
Simulation of current through cap and voltage across it, notice the constant 480mA up until the cap is fully charged to 4.8V (initial condition used again to see the cap charging):
One last thing, make sure you do not use the LM741 in your final circuit, it's completely obsolete. Choose a decent general purpose rail to rail input/output opamp (rail to rail means it can swing all the way to each rail at the output and handle voltages up to each rail at the input, many opamps, including the 741, cannot do this - another departure from the convenient world of ideal components)
It is a current limiter, and the current limit is set by the 12 ohm resistor. The idea is that when enough current flows through that resistor, Q2 is turned on, pulling down the base of Q1, "strangling" it.
If Q2 turns on with a Vbe of, say, 0.7V, then the current is limited to 0.7V/12ohms = 58mA.
To understand it, first imagine that Q2 is not there. Basically Q1 is turned on via its base resistor and lets through as much current as it can. If only there was 'something' that would start turning it off when current reaches a settable amount... and that's where Q2 comes in, and the 12ohm resistor is really a current sensing resistor.
Best Answer
This is an oversimplification.
(DC) Current goes through every path available to it, in proportion to the conductance of that path. And conductance is just the flip side of resistance
$$ G = \frac{1}{R}$$
Ohm's law says, for a resistor
$$I=\frac{V}{R}$$
If you apply 5 V across a 1 megohm resistor, 5 microamps will flow through it.
If you apply 30 V across a 1 megohm resistor, 30 microamps will flow through it.
If it didn't behave that way, we wouldn't call it a resistor.