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Angular motion

In the next two sections, we will discuss angular motion, including angular speeds and accelerations of rotating objects. [Pg.212]

In the previous secdon, we explained the concept of linear speed and acceleradon. Now we will consider variables that define angular motion. Rotadonal modon is also quite common in engineering applicadons. Examples of et jneering components with rotadonal modon include shafts, wheels, gears, drills, pulleys, fim or pump impellets, helicopter blades, hard drives, CD drives. Zip drives, and so on. [Pg.212]

The aver angular speed of a line s ment located on a rotadng objea such as a shaft is defined as the change in its angular position (ai qlar displacement) over the time that it took the line to go throi the angular displacement. [Pg.212]

In pracdce, the angular speed of rotatii objects is measured using a stroboscope or a tachometer. [Pg.213]

To get some idea how fiist some common objects rotate, consider the feUowii examples a dentist s drill runs at 400,000 rpm a current state-of-the-art computer hard drive runs at 7200 rpm the earth goes throug i one complete revolution in 24 hours, thus the rotational speed of earth is 15 d ees per hour or 1 degree every 4 minutes. [Pg.213]


The balance wheel in Problem 3 is driven by a eoiled spring ealled a hairspring. The wheel exeeutes simple hamionie angular motion between the two angular limits shown by the double anow in Problem 3. Its oseillation over the marked exeursion is eomplete every 0.500 s. What is the torsion eonstant k of the spring ... [Pg.129]

This Schrodinger equation relates to the rotation of diatomic and linear polyatomic molecules. It also arises when treating the angular motions of electrons in any spherically symmetric potential... [Pg.33]

As given in Chapter 3, the Schrodinger equation for the angular motion of a rigid (i.e., having fixed bond length R) diatomic molecule is... [Pg.342]

Minorski, N. (1941) Note on the angular motion of ships. Trans. American Society of Mech. Eng., 63, pp. 111-120. [Pg.430]

The Coriolis meter (Figure 6.28) contains a sensor consisting of one or more tubes which are vibrated at their resonant frequency by electromagnetic drivers, and their harmonic vibrations impart an angular motion to the fluid as it passes through the tubes which,... [Pg.267]

Planar Couette flow is difficult to maintain in a steady state. Cylindrical Couette flow is much easier, in which the fluid is contained in the annulus between two cylinders in relative angular motion about their common axes, as shown in Figure 2.8.2. [Pg.188]

An angular motion which requires a large angle of movement to operate the switch (Fig. 5.10). This offers a medium sensitivity to stray magnetic fields and shorter switching distances than method A. [Pg.127]

Figure 4.8. Calculated value of the rms amplitude or local polar libration (<5e2> /2) that satisfies Eq. (4.60) or Eq. (4.61) versus the assumed equilibrium polar angle (e0). The solid lines are the solutions of Eq. (4.60) for the indicated values of the reduced linear dichroism (LDr). The dashed lines are the solutions of Eq. (4.61) for the indicated values of A when the local angulaT motion of the transition dipole is assumed to be isotropic. The dotted lines are the solutions of Eq. (4.61) for the indicated values of A when the local angular motion of the transition dipole is assumed to be purely polar. The intersection of pairs of curves defines the region allowed" by a particular pair of LDr and A values and a particular assumption about the degree of anisotropy of the local angular motion of the transition dipole. If the LDr lies between -0.92 and -1.02, as indicated by experiment, then for isotropic internal motion, e0 = 70.5°, and 1/2 = 0.122 (7°) fall in the allowed region. Figure 4.8. Calculated value of the rms amplitude or local polar libration (<5e2> /2) that satisfies Eq. (4.60) or Eq. (4.61) versus the assumed equilibrium polar angle (e0). The solid lines are the solutions of Eq. (4.60) for the indicated values of the reduced linear dichroism (LDr). The dashed lines are the solutions of Eq. (4.61) for the indicated values of A when the local angulaT motion of the transition dipole is assumed to be isotropic. The dotted lines are the solutions of Eq. (4.61) for the indicated values of A when the local angular motion of the transition dipole is assumed to be purely polar. The intersection of pairs of curves defines the region allowed" by a particular pair of LDr and A values and a particular assumption about the degree of anisotropy of the local angular motion of the transition dipole. If the LDr lies between -0.92 and -1.02, as indicated by experiment, then for isotropic internal motion, e0 = 70.5°, and <i5e2>1/2 = 0.122 (7°) fall in the allowed region.
FPA studies at extremely low binding ratios (1/400-1/700 bp) to assess the DNA motion were carried out on ethidium intercalated in calf thymus121 60) and chicken ied-cell(61) chromatin. Under the conditions of these experiments, ethidium is believed to be intercalated only in the linker DNA, and excitation transfer is believed to be negligible. The amplitude of angular motion, or depolarization, at any given time is much lower than in... [Pg.213]

The results from fitting the anisotropy decay support the above conclusions. Wells and Lakowicz(200) resolved two exponential components in the anisotropy decay. They obtained ro = 0.11, t r = 0.3 ns, rj = 0.15, and t = 18.5 ns for the sample with no added Mg2+, and ro = 0.05, t R = 0.4 ns, r J = 0.17, and t"R = 17.4 ns for a sample with 10 mM Mg2+. Here r 0 and r o are the amplitudes of the fast and slow components. The longer rotational relaxation time corresponds to overall tumbling of the tRNA, although its amplitude is reduced by much more rapid local motions. The shorter relaxation time corresponds directly to a rapid local motion. Upon addition of Mg2+, the relative amplitude of die rapid local motion decreases, while that of the overall tumbling increases. This implies that the wyebutine base is held in a more rigid or constrained state, such as a 3 stack, in the presence of Mg2+. In that state, the amplitude of local angular motion is substantially diminished in comparison with that in the alternate state that prevails in the absence of Mg2+. As noted before, the exact nature of these conformation(s) is unresolved. [Pg.221]

Fig. 212. A diagram of the mechanism for moving the stirrer of a Chaudel-Page kneader in translatory and angular motion, according to Yegorov [11]. Fig. 212. A diagram of the mechanism for moving the stirrer of a Chaudel-Page kneader in translatory and angular motion, according to Yegorov [11].
The rotation rate of the element about the axis perpendicular to the r-z plane (i.e., about the 6 axis) is measured by the angular motion d le of the diagonal line, which is shown dashed in Fig. 2.6. The angular rotation is influenced by both the dilatation and the shearing of the element. The following equations are developed geometrically from Fig. 2.6 ... [Pg.31]

Angular motions (roll, pitch, yaw) 0-7.5 degrees single amplitude... [Pg.113]

Angular Momentum Conservation in Non-radiative Transitions. The very general law of conservation of the angular momentum of any isolated physical system (e.g. atom or molecule) applies to non-radiative as well as to radiative transitions. This is often described as the rule of spin conservation, but this is not strictly accurate since only the total angular momentum must remain constant. Electrons have two such angular motions which are defined by the orbital quantum number L and the spin quantum number S, the total... [Pg.64]

Fiber motion — Jeffery orbits. The motion of ellipsoids in uniform, viscous shear flow of a Newtonian fluid was analyzed by Jeffery [32, 33] in 1922. For a prolate spheroid of aspect ratio a (defined as the ratio between the major axis and the minor axis) in simple shear flow, u°° = (zj), the angular motion of the spheroid is described... [Pg.544]


See other pages where Angular motion is mentioned: [Pg.2456]    [Pg.180]    [Pg.434]    [Pg.618]    [Pg.209]    [Pg.515]    [Pg.361]    [Pg.84]    [Pg.284]    [Pg.104]    [Pg.194]    [Pg.212]    [Pg.214]    [Pg.214]    [Pg.322]    [Pg.326]    [Pg.705]    [Pg.208]    [Pg.64]    [Pg.562]    [Pg.64]    [Pg.65]    [Pg.371]    [Pg.278]    [Pg.302]    [Pg.306]    [Pg.213]    [Pg.76]    [Pg.76]    [Pg.365]    [Pg.85]    [Pg.226]    [Pg.69]    [Pg.133]   
See also in sourсe #XX -- [ Pg.212 , Pg.213 ]




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Angular motion acceleration

Angular motion examples

Angular motion rotational speeds

Orbital Motion and Angular Momentum

Simple harmonic motion angular frequency

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