I said:
"If the coiled coil is straightened out, then the resulting single strand of wire, which will be over a meter long, will have an inductance which is larger than the coiled coil IF IT IS FORMED INTO A CIRCULAR LOOP, OR SMALLER IF FORMED INTO A NARROW HAIRPIN SHAPE"
The filament is a tungsten wire about .0018 inches in diameter. If you straighten it out and form it into a circular loop, the loop will be about 39.37/Pi = 12.5 inches in diameter. The inductance of such a loop is about 1.8 uH. The coiled coil has a measured inductance of about 190 nanohenries.
But, then you ask:
"...why there is a spike ( not inphase with voltage waveform during starting?"
The spike is due to the fact that when the voltage is first applied, the temperature of the filament is at room temperature (about 20 degrees centigrade). But within a short time (milliseconds), the temperature rises several thousand degrees. This causes the resistance to increase by a factor of about 15.
The initial current is about 6 amps, but after several tens of milliseconds, it decreases to about .4 amps.
The inductance hardly changes at all due to the very great increase of temperature.
This very large change in resistance is the dominant effect. The inductance of the filament has a negligible effect on the initial rise time of the current pulse compared with the other circuit inductances.
You say:
"...circuit inductance are always available in the circuit"
This is quite correct, and the circuit inductances don't change as the filament becomes white hot. It is the change in filament resistance that determines the shape of the current pulse vs time.
In one of your posts, you suggest that strictly speaking, the inductance of the filament will have an effect on the current. This is true, but the effect is completely negligible compared to other effects, especially the change in resistance of the filament vs time as it heats up.
The effect of circuit inductances will be seen mainly in the initial rise time of the current pulse, which I measured as about 200 nanoseconds. If the sweep speed of the oscilloscope is set to display 10 milliseconds/centimeter, as in this scope photo:
http://www.freeimagehosting.net/uploads/4463acf782.png
then the rise time of the current pulse appears almost instantaneous, but it is actually about 200 nanoseconds. The circuit inductances have essentially no noticeable effect on the current pulse after the initial rise time. The large decrease in the current occurring in a few milliseconds is due to the increase in the resistance of the filament as its temperature rises to several thousand degrees.