Bosch Automotive Handbook by Bentley Publishers

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Html 2008-1-10 Basic principles, Physics 页码,11/13 stress (example: turbine blades). Relaxation: Reduction of the tension forces and stresses, whereby the initially applied (usually purely elastic) deformation remains constant (see Table 3 for examples). 1 σB) and maximum stresses and temperatures such as are encountered in static relaxation tests, the same deformations and losses of force only occur after a period of load which is approximately 10 times (or more) as long as that of the static relaxation tests.

For retardation to rest, substitute υ2 = 0. html 2008-1-10 Basic principles, Physics 页码,4/14 Angular acceleration α = (ω2 – ω1)/t Numerical relationship: α = π (n2 – n1)/(30t) α in 1/s2, n1 und n2 in min–1, t in s Final angular velocity ω2 = ω1 + α · t Initial angular velocity ω1 = ω2 – α · t For uniformly retarded rotary motion (ω2 is smaller than ω1) ist α is negative. e. 2 %). html 2008-1-10 Basic principles, Physics 页码,6/14 Throwing and falling (see equation symbols) Body thrown vertically upward (neglecting air resistance).

The local stressing can continue to be measured, using foil strain gauges for instance. As an alternative, or for preliminary design purposes, the finite-element method can be applied to calculate numerically the stress distribution and to compare it with the respective limit stress. Creep behavior If materials are subjected for long periods of time to loads at increased temperatures and/or to high stresses, creep or relaxation may occur. html 2008-1-10 Basic principles, Physics 页码,11/13 stress (example: turbine blades).

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