210 likes | 382 Views
This guide provides an overview of electric fields, potential, and energy based on Coulomb's law. It explains electric field strength, the concept of electrical potential, and potential energy of point charges. Formulas such as E = kQ/r² for electric field strength and V = kQ/r for electrical potential are highlighted, along with practical examples involving hydrogen atoms. The text also covers the work done in moving charges between different potentials and introduces equipotential surfaces. Ideal for students seeking clarity on these foundational concepts in electrostatics.
E N D
9: Motion in Fields 9.3 Electrical field, potential and energy
Electric Fields Recap: Coulomb’s law: Electric field strength: F = kQq r2 …the force per unit charge experienced by a small positive point charge placed in the field. E = kQ r2
Electrical Potential It can be shown that... or... Where... V = Electrical potential (Volts or JC-1) r = distance from centre of point charge (m) Q = point charge (Coulombs) k = Coulomb constant = 8.99 x 109 Nm2 C−2 The electrical potential at a point in a field is defined as the work done per unit charge in bringing a positive test charge from infinity to the point in the field. V = kQ r V = 1Q 4πε0 r
E.g. Calculate the potential due to the proton in a hydrogen atom at a distance 0.5 x 10-10m. ( k = 8.99 109 N m2 C-2 ) A: V= 29V
Electric Potential Energy Again it can be shown that... or... The electrical potential energy of a point charge at any point is defined as the work done in moving the charge from infinity to that point. Ep = kQq r Ep = 1Qq 4πε0 r E.g. Calculate the potential energy between the proton in a hydrogen atom and an electron orbiting at radius 0.5 x 10-10m. ( k = 8.99 109 N m2 C-2 ) A: E = -46 x 10-19J
Work done moving a charge If a charge is moved from one point (x) to another (y), where the potential is different, work is done. Work done = Final Ep – Initial Ep = Vyq - Vxq The path taken does not affect the work done. Work done will equal the change in potential energy. x y
Equipotentials Equipotential surfaces also exist in electric fields...
Subtitle Text
Potential gradient Again, this will be equal to the field strength at a point in an electrical field... Work done to move a charge from one potential to another = qΔV But also W = FΔx So... FΔx = qΔV So... E = (-) ΔV Δx
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text
Subtitle Text