2019
DOI: 10.15632/jtam-pl/105465
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Effect of the temporal profile of the friction power on temperature of a pad-disc brake system

Abstract: A mathematical model to analyse the influence of change of the friction power over time on temperature of a pad-disc tribosystem has been proposed. For this purpose, a boundary--value problem of heat conduction for two semi-infinite bodies with taking into account heat generation due to friction on the contact surface has been formulated. Exact solutions of this problem were obtained for seven temporal profiles of the specific heat generation power, which were established experimentally. For selected friction … Show more

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Cited by 13 publications
(16 citation statements)
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“…When increasing the thickness d, the maximum temperature drops and then stabilizes in the range of a d 3, where a = 1.29 mm, 1.17 mm, 1.11 mm for α = 0, 0.5 and 1, respectively. This parameter is a theoretical distance from the heated surface in which the temperature achieves 5% of the maximum value, and it is called the effective depth of heat penetration (Yevtushenko et al, 2019). It should be noted that increasing of the frictional facing thickness d causes more intensive convective heat exchange due to enlargement of the lateral surfaces area.…”
Section: Resultsmentioning
confidence: 99%
“…When increasing the thickness d, the maximum temperature drops and then stabilizes in the range of a d 3, where a = 1.29 mm, 1.17 mm, 1.11 mm for α = 0, 0.5 and 1, respectively. This parameter is a theoretical distance from the heated surface in which the temperature achieves 5% of the maximum value, and it is called the effective depth of heat penetration (Yevtushenko et al, 2019). It should be noted that increasing of the frictional facing thickness d causes more intensive convective heat exchange due to enlargement of the lateral surfaces area.…”
Section: Resultsmentioning
confidence: 99%
“…where is the initial temperature. Solution to the problem (13)- (19) was found based on the following Duhamel's theorem (Ozisik,1993). * ( , ) = ∫ * ( )…”
Section: Fig 1 Scheme Of the Problemmentioning
confidence: 99%
“…In the case of braking, when the time of pressure increase is close to zero, → 0 (11), the solution to the thermal friction problem (13)- (19) has the following form:…”
Section: Fig 1 Scheme Of the Problemmentioning
confidence: 99%
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