IB Prized Writing Sevenoaks School IB Prized Writing 2014 | Page 29

Robert Cinca - Physics had been steady for a while. I then measured the size of the maximum surge current (using the software’s tracer function, which allowed me to look at each recorded point in detail). Measuring the time taken to reach the maximum surge current was also done using the tracer function; however, to measure the surge current time I had to judge where the final steady current was by eye (see below for comment on precision). By varying the resistance in the variable resistor, I was able to plot results for many different final currents. I then repeated my experiment with the second filament bulb I had. Control Variables During my experiment, I had to control some variables in order for my experiment not to be affected. Firstly, I used the same filament bulb for each experiment. In order for there to be a surge current, I waited two minutes (with the circuit turned off) between each measurement in order to let the filament bulb cool down. Whilst doing the experiments, apart from changing the filament bulb (from the 0.15A one to 0.30A one), I kept the same apparatus throughout. Comment on Range Used I used a range of final currents varying from 0.06A to 0.32A. I used the following range because: on the lower end of my results, the percentage uncertainties were becoming too great and the current was taking too long to reach a steady level. On the top end of my results, I was limited by my filament bulbs, which could only take a maximum potential difference of about 8 volts. Even so, my range was sufficiently large enough for me to take lots of readings and be able to plot a reliable graph. Limitations of the experiment On the whole, the experiment was very precise, helped by the use of data studio (which let me take readings every millisecond). The uncertainty in the final current is: ±0.01A. To improve this, I would use a more precise ammeter. The uncertainty of the surge current time was determined by the half range of the experimental results, which varied between ±0.004s and ±0.03s. Though precise, this could be improved further by measuring the changing gradient of the surge current with time. The start of the surge current is determined when the changing gradient of the surge current with time is zero. 28