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Effect of surface roughness combination on frictional sound

机译:表面粗糙度组合对摩擦声的影响

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Whenever two bodies slide against each other in dry contact, they start to vibrate and radiate sound. It is believed that the main cause for such small-scale vibration and sound is the surface roughness. Despite this common recognition, there are only a small number of past experimental studies focused on the effect of surface roughness on friction induced sound. Takahashi [1] studied frictional noise under heavy load, generated by the contact of the rim of a rotating cylinder against a plate specimen (R{sub}(max)<0.5μm). For two different cylinders with R{sub}(max) roughness of 0.2 and 3 pm, sliding against the plate in the presence of spindle oil, he observed that the change in the sound pressure level (SPL) is proportional to 2Olog{sub}10(R{sub}(max2)/ R{sub}(max1)) Later Yokoi and Nakai conducted experiments on a spherical tip pin-on-rim apparatus in dry contact. They used three different disks with roughness R{sub}(max) = 5, 3 and 0.5 μm (pin roughness not specified), and modified Takahashi's relationship, so that the difference in SPL was equal to 20log{sub}10(R{sub}(max2)/ R{sub}(max1)){sup}0.8. In a later study Othman et al. investigated the frictional noise generated when a sharp stylus traversed the rough surface of a flat disk at high speed (1.05 m/s). They used disks made of brass, aluminium and steel with average surface roughness R{sub}a in the range of 1.5 to 20 μm, and found that SPL and surface roughness are related by the expression: R{sub}a = C(SPL){sup}h, where C and b is an experimental parameters, b depending on the material. In essence, Takahashi proposed a linear relationship between sound pressure and surface roughness for lubricated hertzian line contact. Yokoi and Nakai modified it for dry hertzian point contact to a power law with power (of 0.8 - still very close to linear relationship. The formula proposed by Othman et al. for dry point contact at high speed describes a base 10 exponential dependence of sound pressure on the surface roughness.
机译:每当两个身体在干燥接触中彼此滑移时,它们开始振动并辐射声音。据信,这种小规模振动和声音的主要原因是表面粗糙度。尽管存在这种共同识别,但只有少数过去的实验研究集中于表面粗糙度对摩擦诱导声音的影响。 Takahashi [1]通过旋转圆柱的边缘与板标本(R {sub}(MAX)<0.5μm)的触头产生重载的摩擦噪声。对于具有0.2和3μm的R {Sub}(MAX)粗糙度的两个不同的汽缸,在主轴油的存在下滑动在板上,他观察到声压水平(SPL)的变化与2olog {sub}成比例10(R {sub}(max2)/ r {sub}(max1))以后yokoi和nakai在干燥接触的球形尖端销上销上进行实验。他们使用了三种不同的磁盘与粗糙度R {子}(最大)= 5,3和0.5微米(销粗糙度不指定),和修饰的高桥的关系,使得在SPL差等于20log {子} 10(R {子}(max2)/ r {sub}(max1)){sup} 0.8。在后来的研究中奥曼等人。在高速(1.05米/秒)的尖锐钻石穿过扁平盘的粗糙表面时,调查摩擦噪声。它们使用了由黄铜,铝和钢制成的盘,平均表面粗糙度r {sub} a在1.5至20μm的范围内,发现SPL和表面粗糙度与表达式有关:R {sub} a = c(spl ){sup} h,其中c和b是实验参数,b取决于材料。实质上,Takahashi提出了用于润滑的Hertzian线路接触的声压和表面粗糙度之间的线性关系。 Yokoi和Nakai将其修改为干燥的Hertzian Point与电力法的电力法(0.8 =仍然非常接近线性关系。Othman等人提出的公式。对于高速的干燥点接触描述了声音的基本10指数依赖性表面粗糙度的压力。

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