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Chapter 1: Introduction, Vector Functions and Electrostatics

131 words

Vector functions are simply functions that can be expressed like this:

F(x,y,z)=Fx(x,y,z)i^+Fy(x,y,z)j^+Fz(x,y,z)k^.\mathbf{F}(x, y, z) = F_x(x, y, z) \hat{i} + F_y(x, y, z) \hat{j} + F_z(x, y, z) \hat{k}.

They specify a magnitude and direction for every point (x,y,z)(x, y, z).

A fundamental property of nature is “charge”. There are two kinds of charge - positive/negative.

Coulomb’s law states that the force between two charges qq and q0q_0 is:

Fq=14πϵ0qq0r2u^\mathbf{F_q} = \frac{1}{4 \pi \epsilon_0} \frac{qq_0}{r^2} \hat{u}

where u^\hat{u} points from q0q_0 to qq.

The Electric field is defined by:

E=Fqq.\mathbf{E} = \frac{\mathbf{F_q}}{q}.

Another very important property is superposition. Superposition states that the presence of other forces does not affect the original force itself, allowing us to simply add forces vectorially.