Equation 19-9 and the field properties shown in Figure 19-17 are strictly correct only if the wire is infinitely long. But they are very good approximations if the distance \(r\) is small compared to the length of the wire.
The constant \(\mu_0\) in Equation 19-9, called the permeability of free space for historic reasons, plays a role in magnetism that’s comparable to the role of the constant \(\epsilon_0\), the permittivity of free space, in electricity (see Section 16-6). Its value is exactly \(\mu_0 = 4\pi \times 10^{-7}\ \mathrm{T} \cdot \mathrm{m}/\mathrm{A}\).