The resolving power of a telescope with a primary lens/mirror of diameter
\[D\]
using electromagnetic radiation of wavelength \[\lambda\]
is given by the Rayleigh criterion \[\theta \simeq \frac{1.22 \lambda}{D}\]
, so we can resolve objects an angular distance \[\theta\]
apart using this interferometer and this wavelengthradio waves are radio waves of very long wavelength. Light emitted from distant objects is red shifted into the radio part of the spectrum in reaching us. This means that we can only really study these objects at radio wavelengths, and must use interferometers with a large baseline
\[D\]
to be able to resolve them and determine the source of the radiation.