Does this Resonate?
Distortion Causes
Tu-be or Not Tu-be
Normally about 15 minutes idle is necessary to optimize the ST-10✝ sonics. July 2018: Zero Rain, Sunny. Media Room very warm. Extended sessions with robust program added an edge to the ST-10✝. The case temperature climbed above 40°C from the normal low 30's, indicating higher internal temperatures. We put the PL5 in its stead. Normally, the PL5 takes about 30 minutes to warm and the sonics stabilize. In the summer heat, almost immediately
Heat Kills
Heat is a killer. But, it takes surprisingly little air to keep most components cool. I discovered this in the early 70's on a Yamaha Class A amp. Passively cooled, it was too hot to touch and component life, particularly electrolytic caps, would be short. Adding a thermostatically controlled fan that barely ticked over kept the beast cool.
The PL5 gets very warm, as do most uncooled tube amps. Adding
The Fly in the Ointment...
About 1% of the applied energy is radiated as sound and the rest converted to heat in the voice coil and crossover components. Crossover frequency will shift and output level will decrease due to increased R. Graph shows effect of copper voice coil heating [0.395%/°C] and crossover frequency for a 2KHz 2nd order filter. Effects of crossover component heating ignored.
Coils for various drivers do not heat equally, so an initial 2KHz calculated @ 20°C could become 1850z @ 40°C for the woofer and 1925Hz @ 30°C for the tweeter. Degree of heating is program and level dependent. The blue trace in the first graph is the theoretical woofer attenuation due to the increased resistance. However this new resistance changes the impedance only slightly. This new impedance will interact with the cable and further adjust frequency and phase response.
The 2nd graph shows how the impedance swamps the expected attenuation from R alone, dropping only about 1/2 of the expected value from the first graph. The third graph shows the phase response.
See Stereophile's
Hot Stuff: Loudspeaker Voice-Coil Temperatures and 1992 AES paper
Heat Dissipation and Power Compression in Loudspeakers for further reading.