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Joule: J V C The unit of energy, the familiar joule, is also used for electrical energy. The joule provides a crossover point between mechanical and electrical measurements. One joule is the energy needed to move one coulomb of charge up one volt of electrical potential. It is also de ned as the amount of work performed by a current of one amp acting against a resistance of one ohm for one second. Resistance is discussed in the next chapter.

Fig 613: The reliability factor, Kr, for ball and roller bearings [13]



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L 10 Creq = Fr K r LR In order to consider the influence of the axial load, the radial load, Fr, and the thrust load, Ft, are combined to give a pure radial equivalent load, Fe, that is used to approximate the life of the bearing The pure radial equivalent load also considers the contact angle, and this results in the following set of equations: Radial ball bearings with an angle of contact, a = 0

Watt: W V I Work or power is represented by the Watt, which is a function of voltage and current. The watt could also be considered joules per second, W J/s.

Rolling Element, Hydrodynamic and Hydrostatic Bearings Angular contact ball bearings with an angle of contact, a = 25 For 0 <





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The influence of shock loading can be taken into account by using the application factor, Ka, given in Table 65 for various degrees of shock loading The nominal load will be increased by the application factor By taking axial load and shock loading into consideration, the bearing life equation is further modified as [13]

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This discussion of electricity has focused on the ow (current) and pressure (voltage) of the electric charges. The question is then, how do we create this voltage With electron pumps. The electricity that comes out of the walls in your house is pumped there by giant generators. These generators use magnets to push the electrons around. Batteries do the same thing but on a smaller scale and without magnets. Inside the battery is a chemical paste that acts as a pump. As the chemical reaction inside the battery goes forwards, it charges its terminals. Batteries are like chemical springs unwinding, converting chemical potential energy into electrical energy. When you recharge a battery, you are rewinding this chemical spring. Inside a battery, a chemical redox (reduction/oxidation) reaction occurs at two electrodes, or conductive posts, which are separated by a conductive uid or paste, the electrolyte. The reduction reaction occurs at the cathode, which is the positive electrode. The oxidation reaction occurs at the anode, which is the negative electrode.

Application factor, Ka [13]

As the battery discharges, powering your circuit, the anode oxidizes (picks up oxygen) and creates a surplus of electrons These electrons then ow through your circuit (the load) and reenter the battery at the cathode They can get back in through the cathode because it is performing the reduction reaction (losing oxygen), which combines the electrons with the cathode The electrolyte that bathes both the anode and cathode nishes this electron loop, allowing the electrons to hitch a ride to the anode for another trip through the oxidation reaction Note that batteries don t create electrons; they just provide a way to move them around Of course it s far more complicated than that It s not just electrons, the negatively charged particles, that move Protons also ow in the electrolyte, and the chemical reactions are fairly complicated.

The service life of a given bearing in revolutions can now be calculated by using the following relationship:

C 3 Lrevolutions = K r L R Fe K a If the bearing works at constant speeds of nrpm, it is then possible to calculate the service life in hours by modifying the preceding equation as

What remains to be done is to compute r;;(p', p). We shall satisfy ourselves with the case where p and p' are on-shell and r p is to be considered as sandwiched between Dirac spinors as ii(p')rp(p', p)u(p). We shall, however, not write the spinors explicitly but we freely use the Gordon relation

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