On the Boundary between Nonlinear Jump Phenomenon and Linear Response of Hypoid Gear Dynamics

<table>Dynamic mesh force (STD) for <svg height="20.924999" id="M125" style="vertical-align:-4.74141pt" version="1.1" viewbox="0 0 63.9375 20.924999" width="63.9375" xmlns="http://www.w3.org/2000/svg">
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<tspan style="font-size: 12.50px; " x="-0.94" y="2.54">𝑇</tspan>
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<tspan style="font-size: 8.75px; " x="0" y="0">𝑝</tspan>
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<tspan style="font-size: 12.50px; " x="0" y="0">=</tspan>
<tspan style="font-size: 12.50px; " x="12.027886" y="0">2</tspan>
<tspan style="font-size: 12.50px; " x="18.279387" y="0">.</tspan>
<tspan style="font-size: 12.50px; " x="21.405136" y="0">0</tspan>
<tspan style="font-size: 12.50px; " x="27.656635" y="0">1</tspan>
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</svg>. *, <span style="font-family:monospace">□ </span>no impact;<i> •</i>, <span style="font-family:monospace">○ </span>single-sided impact; +: <span style="font-family:monospace"><i>▽</i></span> double-sided impact;  ––-: dynamic mesh force (RMS) for increasing frequency; …: dynamic mesh force (RMS) for decreasing frequency; - - -: <i>theoretical </i>static mesh force.</table>

Advances in Acoustics and Vibration

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Figure 7

Figure 7: On the Boundary between Nonlinear Jump Phenomenon and Linear Response of Hypoid Gear Dynamics 