Wednesday, November 5, 2014

The Potential Difference Due to Continuous Charge Distributions, Electric Potential due to a finite-length line-charge, Electric Potential Lab/Activity


The Potential Difference Due to Continuous Charge Distributions


A ring of charge has a total charge of Q = 20 µC (or 20 ´ 10-6 C).  The radius of the ring, a, is 30 cm.  We wanted to find the electric field, E, at a distance of x cm from the ring along an axis that is perpendicular to the ring and passing through its center and the potential, V.   First we divided the ring into 20 pieces of charge Dq and calculated the total V at a distance of x = 20 cm from the center of the ring using a spreadsheet program.  We calclulated the potential difference to be 4.7 x 10 ^ 5. We then integrated to find a more exact value of the total potential difference.  We determined that the potential difference was 4.9 x 10 ^ 5.  There is a 4.16% difference between the two values which is due to the face that we only split the ring into 20 pieces when calculating it whereas the integral takes an infinite amount of pieces and sums them.














Electric Potential due to a finite-length line-charge



A 16.0 cm long, horizontal rod has a uniform charge density of 2.70 mC/cm. Taking the left end of the rod to be the origin determine the electric potential at the point (10.0 cm, 15.0 cm).  First we divided the bar into 17 equal pieces from .005 m to .165m and calculated the electric potential by using the equation kq/r where r = sqrt((a-x)^2+b^2) for each of the 17 pieces and then summed them up to get the total electric potential of 2.63 kV  We then calculated the electric potential by integrating. We found that value to be 2.47kV.




















Electric Potential Lab/Activity


See pictures  








solving V/m & V/cm












No comments:

Post a Comment