Mapping The Electrostatic Potential And Electric Fiel 463458
Mapping The Electrostatic Potential And Electric Field1mapping The E
Mapping The Electrostatic Potential and Electric Field
Introduction This lab's objective is to examine potentials, equipotential curves, and electric field caused by two-dimensional electrostatic charge distribution. The electric force is conservative. We exploit this fact and consider the force to be associated with electric potential V. it is extremely difficult to measure electric fields directly.
Procedure Apparatus i. Voltage meter ii. Electrodes iii. Meter probes iv. D.C. Power supply v. Conducting paper vi. Power supply wires
Procedure Part I: Point Source and Guard Ring The reference line amid the source point and guard ring was drawn—reference probe set at the guard ring, a region that comprises of negative charges. A potential difference of 5V was applied, and the potential difference between the probe measured after every 2mm, starting the guard ring.
Part II: Mapping Potential Dipole After setting up the right electric dipole configuration followed by the application of 5V potential difference between the two electrodes, a reference probe was placed at the midpoint of the two electrodes. Equipotential curves and electric field lines were created, and configuration mapped inside the boxed space.
Part III: Like Charges in a Box After the suitable electronic configuration was set up using two positive charges and a potential of 5V applied amid the electrodes, the reference probe was situated relatively in the middle. The equipotential curves and electric field lines were drawn at different points created by the configuration, and they were mapped.
Part IV: Parallel Plates The equipment was set up, as shown in the figure above, and the potential of 5.00 V applied across the electrodes. A reference line was drawn at the midpoint of the plates, and a negative electrode was set as the reference point.
The potential difference between the probes was measured every 0.5 cm along the reference line, beginning from the negative electrode's 0.5cm mark. The measurement moved closer until the difference was zero.
Precautions and Sources of Error Data, Calculations, and Fittings Part 1 Distance (m) Potential (V) 0....................777 Graph of voltage vs. Distance for point Part II Electric field lines are normal to the equipotential lines. Part III There is a high potential close to charges and low potential as one moves far away from the charges. The electric field is also seen to be perpendicular to equipotential. Part IV Data for point source and guard ring Distance (m) Potential (V) 0..............5 Graph Possible Sources of Errors The absence of data points taken for potential differences can enhance inaccuracy in potential difference vs. distance graph also, constant fluctuation in multimeter results in the inability to offer precise potential value.
Questions
- Any reference point that lies within the parallel lines results in an equipotential similar to parallel plates. The potential
- If a different reference point were selected, any reference point within the lines would eventually result in equipotential since plates are parallel.
- No. The potential does not vary. This is because there is no interaction between the positive and the negative charges.
- Equipotential lines look like curves that progress in half circles. The unique equipotential line is the one that is vertically right in the middle of the two charges.
- The potential is furthest from the relative halfway point while it's very close to the positive electrodes. Potential does not vary outside the box because the box creates a boundary of the electric field.
- About the graph, an increase in distance results in a decrease in potential. Potential and inverse are inversely proportional—an increase in distance results in a decrease in potential.
Conclusion
The experiment enhances familiarity in the discipline of the electric field as well as equipotential curves that result from charges. This is best understood by mapping the lines in many configurations. The students also enhance their skills necessary in connecting simple circuits.
Mapping The Electrostatic Potential And Electric Field
This experiment demonstrates fundamental principles of electrostatics through systematic mapping of potential and electric field configurations. Students observe how charges influence the surrounding space, visualize equipotential lines and electric field vectors, and develop an intuitive understanding of the electrostatic phenomena that govern many practical and theoretical applications. Mapping the electrostatic potential and electric field is integral to fields such as electrical engineering, physics, and applied sciences, providing insights into charge distribution and field behavior.
References
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