(The Dipole Field Along the Dipole Axis)
A proton and an electron separated by 2 × 10^{−10} m form an electric dipole, see Fig. 20.10. Use exact and approximate formulae to calculate the electric field on the x-axis at a distance 20 × 10^{−10} m to the right of the dipole’s center.
In this problem we have a = 10^{−10} m, q = e = 1.6 × 10^{−19} C, x = 20 × 10^{−10} m, ke = (9 × 10^{9} N.m^{2}/C^{2}) (1.6 × 10^{−19} C) = 1.44 × 10^{−9} N.m^{2}/C, x − a = 19 × 10^{−10} m, and x + a = 21 × 10^{−10} m. Using the exact formula given by Eq. 20.11 in the case of x > +a, we have:
=(1.44\times10^{-9}\,\mathrm{N.m^{2}/C})\left[\frac{1}{(19\times10^{-10}\,{\mathrm{m}})^{2}}-\frac{1}{(21\times10^{-10}\,{\mathrm{m}})^{2}}\right]
= (1.44 × 10^{−9} N.m^{2}/C)[2.770 × 10^{17} m^{−2} − 2.268 × 10^{17}m^{−2}]
= 7.236 × 10^{7} N/C
On the other hand, we have x >> a and we can use the approximate formula given by Eq. 20.13 as follows:
\vec{E}=\left\{\begin{matrix}2 \ k\frac{\vec{P}}{x^{3}}& x>>a\\2 \ k\frac{\vec{P}}{|x|^{3}}& x<<-a \end{matrix} \right. \quad (\vec{p} = 2 a q \vec{i}) \qquad (20.13)
E=2k{\frac{p}{x^{3}}}=2k{\frac{2a \ e}{x^{3}}}=k e\frac{4a}{x^{3}}=(1.44\times10^{-9}\,\mathrm{N.m^{2}/C})\frac{(4\times10^{-10}\,\mathrm{m})}{(20\times10^{-10}\,\mathrm{m})^{3}}
=7.200\times10^{7}{\mathrm{~N/C}}
Clearly this calculation is a good approximation when x/a = 20.