Hi.
So you give somebody a big lecture about propagation velocity and provide three examples, two of which are absolute and one of which is relative to light.
Not too rigorous if you ask me.
Let me put it in simple language so you can understand better, hopefully.
Let me give you a table of common wire insulation (e) vs propagation velocity (v.c.) vs transit time relative of light speed:-
insulation e v.c. wave transit time relative to light speed (1)
(1) still air 0 0.95 1.06
(2) PE (foamed) 1.55 0.80 1.27
(3) PE 2.26 0.659 1.54
(4) Teflon (TFE & FEP) 2.00 0.70 1.45
(5) PP (polypropylene) 2.10 0.69 1.47
(6) Rubber (Butyl) 2.35 0.653 1.56
(7) Silicone rubber (SE972) 3.16 0.563 1.80
(

PVC 4.00 0.50 2.03
(9) Rubber (Buna S) 2.90 0.587 1.73
(10) Nylon 3.00 0.578 1.76
(11) Neoprene 5.00 0.446 2.28
All above figures are subject to varying slightly as per the relative humidity, frequencies used to do the measurement, & method used to support the centre of the conductor.
For electronic cables, the common compounds used to extrude the insulation are (2),(3),(4), & (

. The others are commonly used for power cables.
Due to its excellent wave propagation property, being second to air (which means bare conductor without insulation), foamed Polyethylene is commonly used for coaxial cable insulation for RF application.
Sorta O.T.:- with this insulation property line-up in mind, I built ALL my audio interconnects using 4N pure silver conductors with AIR as each conductor's insulation which is next best to vacuum.
Guess how I have done it?
c-J
PS: JN: the context I took out from the 'cook book' of an American wire & cable manufacturer established since 1950. It is not Belden, for sure.