1: Electrostatic Fields
- Page ID
- 17289
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- 1.1: Charges and Static Electric Forces
- The electric force is the fundamental force behind nearly every macroscopic force we studied in classical mechanics.
- 1.2: Electric Field
- Originally intended as merely an "explanation" of action-at-a-distance, the idea of an electric field turns out to be a much more useful model than one might expect.
- 1.3: Computing Electric Fields for Known Charge Distributions
- When we encounter electric charges in the real world, they appear in very great numbers. This allows us to treat them as approximately a continuous distribution, making integral calculus a powerful tool for field calculation.
- 1.4: Dipoles
- Particles we encounter (such as atoms and molecules) rarely are electrically charged, as they tend to attract and bond with other particles that are oppositely-charged. But these neutrally-charged particles are still affected by electric fields, thanks to their component charges being ever-so-slightly separated.
- 1.5: Conductors
- It is useful to model materials as one of two types: Those that allow charges to flow freely through them, and those that do not. Here we will examine properties of the former.
- 1.6: Gauss's Law
- The only link we have seen between charge and electric field is Coulomb's law, coupled with the principle of superposition. It turns out that these two quantities have a much deeper relationship, which can be exploited to solve problems in a manner easier than what we have seen so far.
- 1.7: Using Gauss's Law
- Gauss's law has a number of practical uses, such as computing electric fields for highly-symmetric situations, and dealing with conducting shells.
- 1.8: Method of Images
- We develop a trick that allows us to discuss forces and fields that result from bringing free charges near flat plane conductors.