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CHAPTER ISHORT AND SLENDER AIRCOLUMNS CIRCUITS WITHOUT EXPLICIT CAPACITY 1 Circuits Figs I to 5
Survey in pitch Figs 6 to 10 a 4 Continuous change of phase difference Fig n
Phase difference apparently passing through zero Figs 12 to 14
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0.i microfarad acoustic pressure actual adjustment air-currents amplitude bore break capacity cells circuit coefficient coil computed cone constant corresponding crests and troughs cusps cylindrical decrease diameter effect efficiency electric oscillation electrode electromotive force embouchure equation excess experiments farad frequency fringe displacement further given in figure glass pin-hole harmonic Hence henry horn increases indicated inductance induction coil inductor initial insert intersection iron core larger latter linear maxima maximum mercury method millihenry minima minimum moreover nearly negative nodal intensity node observed obtained ohms outer pin-hole overtones parallel phase phase-graph pin-hole probe pipe tt pitch plate pin-hole position preceding preceding graph primary probably punctured quill quill-tube length reduced reentrant relatively resistance resonance reversed salient secondary seems sensitive sequence curve sequence graph sharp shows spring-break stopcock telephone telephone-plate tube tuning U-tube usual values varied vibration vorticity Wimshurst machine zero