sophiecentaur said:
You have managed to confuse me all over again with some of the things you've been writing. Yes. "Due to its shock waves" but the source doesn't appear to say that the boom carpet is a shock wave. My problem with what you say is that the angle of the cone (not sure what to call it after your comment) shows that the speed of the wave front must be less than the plane speed. Wiki tells us the speed of the wave is the speed of sound so is that a shock wave? On the rare occasions (once a year, here) that we hear a boom, the likely offender is a very long way away. That confirms the claims that the speed is not excessive.
Blowing out windows is a very hit and miss phenomenon, depending on the angle, the volume of the building and the way the wave couples to it. I remember a Readers' Digest article (there's a good reference, lol) describing how, during a very early supersonic flight, all the windows on a long, single story airfield building blew out as the wave found its way into a corridor, parallel with the flight path. But you don't need a lot of pressure to do that. We don't have many mechanical sources that are as big as a shock wave from a plane so it's hard to think of examples of Booms that are from any other source but a low volume sound alike can be produced from a sub woofer.
Shock waves travel faster than the speed of sound normal to their length. That's about as fundamental to shocks as it gets. If the Mach number based on the velocity component of the flow approaching normal to the wave is not greater than unity, you cannot have a shock. It follows, then, that the Mach number of the flow approaching any
oblique shock (such as those emanating from an aircraft) must also be supersonic (triangle inequality). Thus, any shock wave propagates faster than the speed of sound relative to the gas approaching it (or, alternatively, relative to the gas into which it is propagating).
The cone you shared above in #13 is not a shock wave. It is, in fact, a Mach cone illustrating the concept of Mach waves and the Mach angle. It is essentially an illustration/extension of the Doppler effect when the sound source is moving at a supersonic speed.
The wave shown in #9 is a shock wave. Near the leading edge, it is what we call a bow shock (or detached oblique shock). That curved region eventually transitions into a more standard oblique shock. Those shocks will propagate a considerable distance from their point of origin.
The Mach angle is defined very simply and is based on the speed of sound waves propagating relative to a supersonic source. It is
\mu = \arcsin\frac{1}{M_1}
where ##M## is the inflow Mach number. In contrast, the shock angle is defined very differently. For a simple 2D wedge, it is common to use the ##\theta##-##\beta##-##M## equation, which is quadratic in ##M_1^2## and depends on ##\theta## (the flow turning angle or wedge angle) and ##\beta## (the shock angle).
\tan\theta = 2\cot\beta\frac{M_1^2\sin^2\beta - 1}{M_1^2\left( \gamma + \cos 2\beta \right) + 2}.
Clearly, ##\beta\neq\mu##. Additionally, ##\beta > \mu## and ##\mu + \theta > \beta##. Finally,
\lim_{\theta\to 0}\beta = \mu.
The schematic below from Wikimedia commons (and the
oblique shock Wikipedia page) lays out the variables. Note that ##\gamma = c_p/c_v## is the ratio of specific heats of the gas.
I will note that the ##\theta##-##\beta##-##M## does not work for conical flows, so you have to use the more complicated
Taylor-Maccoll equations to solve for ##\beta## in that case, though the answers are similar to those for a wedge.
A typical supersonic aircraft might be simplified just to the nose cone. For simplicity, let's just assume it's a blunted right circular cone. A bow shock will form at the tip which will transition to a conical shock wave with angle ##\beta## according to the Taylor-Maccoll equations. This shock will propagate for a great distance (for as long as there needs to be a corresponding change in the direction of the flow) and will travel with the speed of the aircraft since it is attached to and continuously generated by it.