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Mechanical loads inertia

When sizing the VFD to match the connected mechanical load, the foremost consideration is inertia, which is a measure of an object s resistance to changes in speed, whether that object is at rest or moving at a constant speed. This speed can either be hnear (feet per minute, ft/min) or rotational (revolutions per minute, r/min). [Pg.658]

The speed of rotation establishes the cycle time and this, being an important design parameter, is limited mechanically by the mass inertia of the swinging pan and its wet cake load at the point... [Pg.229]

El theory In all materials (plastics, metals, wood, etc.) elementary mechanical theory demonstrates that some shapes resist deformation from external loads. This phenomenon stems from the basic physical fact that deformation in beam or sheet sections depends upon the mathematical product of the modulus of elasticity (E) and the moment of inertia (I), commonly expressed as EL This theory has been applied to many different constructions including sandwich panels. [Pg.635]

The control of dynamic effects at impact rates up to 1 m/s (in some instances somewhat higher) frequently makes use of mechanical damping in the load transmission by placing a soft pad (elastomer or grease) between the striker tup and the specimen [3,5], Above about 1 m/s inertia effects overshadow the true mechanical response of the specimen. Due to such dynamic effects, the applicability of FBA is limited to loading rates up to about 1 to 2 m/s for bending type fracture specimens. [Pg.192]

The bond graph model of the nominal system in integral causality is given in Fig. 3.18. The mechanical part of the engine is characterized by the viscous friction fm and inertia Jm- Load part is characterized by friction fs and inertia Js. Reducer part is represented by TF, and the axles stiffness at the input and output of the reducer is represented by C 1/K element. Modulated effort sources d and (U are the disturbing torques caused by the presence of the backlash. Axle velocities are represented on the bond graph model of Fig. 3.18 by two flow sensors Df % and Df ... [Pg.124]

The inverse bond graph is obtained from the direct bond graph (Fig. 4.11) by replacing each of the two effort sources representing the voltage source and the external moment by a flow source-effort sensor, SS, as depicted in Fig. 4.24. The source-sensor elements lead to differential causality at the ports of the two I elements accounting for the self-inductance La of the rotor winding and the mechanical inertia Jm of rotor and load. That is, the inverse model has no states. Hence, the denominator of all transfer functions of the inverse model is a constant. [Pg.164]

Centrifuge model test is to carry the Hn reduced-scale model test in the space with ng inertia. This test method can make the model and the prototype have equal stress and strain, similar deformation and failure mechanism. It is very useful in simulating the characteristic of geotechnical engineering where the self-weight acts as the main load. [Pg.265]

In considering whether a machine is of good mechanical construction, regard must be given to the stresses imposed upon the item when used for its intended purpose and to any additional stresses that could conceivably be imposed upon the item during normal use, due to impact loading, excessive vibration, inertia forces or temperature (both elevated or sub-zero). [Pg.643]

Consider a linear elastic continuum, which may consist of passive and active, i. e. adaptronic, elements. The dynamic equilibrium of the structure can be formulated using the principle of virtual displacements [9] including inertia loads. To express the internal strain energy in terms of displacement variables, the kinematics of the structure has to be considered. Various types of mechanical structures, e. g. beams, plates, or shells, are defined by kinematics relations and constraints. [Pg.79]

Remark 3.5. A mechanical system of rigid parts in accelerated motion will be in equilibrium if the virtual work of the actual impressed and inertia loads for arbitrary admissible virtual displacements vanishes. [Pg.36]

Since beam theory is concerned with the representation of structures with essentially one dimension of extent, the mechanical and electric loads applied to volumes and areas in Eq. (3.62) need to be assigned to the beam reference line. The virtual work (5V (f) of such loads will be defined subsequently and, furthermore, the virtual work of inertia loads will be derived... [Pg.147]

The underlying mechanical degrees of freedom u (x, t) are given by Eq. (8.26). The matrices G(a , t) and G(x, t) contain the initial internal loads to be determined with the aid of Eqs. (8.43). They depend on the initial external loads n x,t), which in turn are composed of the applied external loads h x,t) and those rotational effects that concern the initial state. The latter have been obtained implicitly within the derivation of the virtual work of inertia loads. They are marked in Eq. (8.33), and consequently the initial external loads are given by... [Pg.154]


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See also in sourсe #XX -- [ Pg.148 ]




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