houlahound said:
So power in a light is proportional to diameter of filament assuming constant length tungsten filament?
I'm not sure which element of the thread this has come from - Ohm's ratio, temperature dependence, power in a resistor? But whichever it is, perhaps we need to be clear about the details of the context, else statements like this are hard to evaluate.
Assuming for the moment, it is talking about the light FROM an incandescent bulb, plugged into mains - approximating a constant voltage source, then I would think that:
increasing the diameter would lower the resistance in inverse proportion to the cross sectional area, so inverse proportion to the square of the diameter;
reducing the resistance increases the power dissipation according to V
2/R, so inversely proportional to the resistance or proportional to the are or the square of the diameter;
greater power dissipation would increase the temperature until the radiated power equalled the new electrical power;
since the radiated power is also proportional to the surface area, which is proportional to the square of the diameter, so there is no need for any temperature rise to increase the radiated power.
Net result, increased light power is proportional to square of diameter for a constant length filament, so long as the the resistance of the filament remains much larger than the resistance of the power supply. (If you carry on increasing the diameter of your filament, eventually nearly all the power is dissipated in the supply and very little in the filament - or massive metal bar, as it might then be called.) The temperature does not change (if the filament is in empty space) so the colour does not change.