Radio frequency currents flow largely along the surface of a conductor due to skin effect. As a result, the center portion of a conductor typically plays no role in the conduction of RF current. The conductor can be hollow or filled with any other material and it will have minimal effect, provided the surface conductor is sufficiently thick.
Your telescoping antenna also exhibits skin effect. As a result, the part that is telescoped inside another section plays no practical role in conducting RF current to your SDR antenna input - it is as if it is not even there. Only the visible, outside surface of the telescoping element functions as the antenna.
When configuring a dipole antenna, the overall length in meters is given as:
$$l=\frac{142.5}{f} \tag 1$$
where $f$ is the frequency in MHz.
Equivalently, the length of a dipole in feet is given as:
$$l=\frac{468}{f} \tag 2$$
The length of each leg is one half of $l$. The length is typically not extremely critical for receive applications.
The NOAA APT transmissions are right hand circularly polarized satellite signals (RHCP). The dipole antenna is linearly polarized. As a result you will experience about 3 dB of signal loss. This is typically an acceptable loss for this application. Keep your dipole antenna horizontally orientated and at least 1 meter away from other objects including the earth. Turn it about the vertical axis that is perpendicular to the telescoping elements for the best signal strength.