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Here is a way to visualize and help you understand the basics.
Consider a Y connected resistive load for your heater. For a balanced load each of the three resistors dissipates 1/3 of the power. Beacuse of the Y connection the current in the supply line is equal in magnitude and in phase with the current in its connected resistor.This should be intuitively obvious.
The "leg to leg" to "leg to nuetral" ratio can be determined by a vector diagram where "leg to leg" = 2 * "leg to nuetral" * sin 60 = 2 * 0.866 * "leg to nuetral" = 1.732 * "leg to nuetral". Therefore, for your 208 supply the "leg to nuetral" = 120.09, but 120 is a number you should have already known, and thus you would know that ratio or could calculate it.
From the above it should be obvious that you divide total watts by 3 to get the dissipation in one resistor of the Y load, then divide that wattage by 120 to get the current is one supply line. Writing an equation for this we have I * V / 1.732 = W/3. It should be noted that the exact value of 2 * sin 60 = sq-root of 3. But 1.732 is quite close and it is the year of George Washington' birthday to help you remember. Now you see the final equation becomes I = W/(1.732*V) = 0.577*W/V. Where I is line current, V is leg to leg voltage, and W is total power of the heater.
If you can remember this train of thought you might in the future be able to derive the the equation yourself.
It is not true that the phase angle of the current in one element of a delta load is in phase with the line current. So if the question had been posed as a delta load that might have been a tricker question because it might have thrown you off. You might not have considered changing the load to a Y to force the line current phase angle to equal load current phase angle.
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