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Impulse of the force

Consider an inelastic collision between two smooth identical spherical particles 1 and 2, of mass m and diameter dp = d 2 [32] [60]. If J12 is the impulse of the force exerted by particle 1 on particle 2, the linear momentum balances over a collision relate the velocity vectors of the center of each sphere just before and after the collision through ... [Pg.515]

It is required that the component of the relative velocity perpendicular to the apse line should be unchanged in a collision, thus the impulse J12 must act entirely in the k direction. On this demand, J12 can be determined from (4.21), (4.22) and (2.123). The impulse of the force exerted by particle 1 on particle 2 is given by ... [Pg.515]

Bones must be thought of as more like plastic than like stone. They have a good deal of flexibility and can accommodate and distribute stresses within a certain capacity of tolerance. The amount, interval, and impulse of the force, as well as the vector, direction, and individual structure, age, and nutritional status of the bone help to determine the result. Sudden forces may create bending, as in a green-stick fracture in children, or rapture of the components and related structures. Sometimes the force is transmitted to smrounding or imderlying structures of other types. It is difficult to conceive of any instance when a fracture of bone does not involve also soft tissue injmy of the regional structures. [Pg.97]

The impulse of the force exerted by particle 1 on particle 2 is given by ... [Pg.554]

We derive the concept of the dynamic efficiency of the air curtain, E, which is equivalent to the ratio between aerostatic pressure forces affecting the gate aperture and the doubled initial impulse of the air curtain jets ... [Pg.561]

To change an object s speed it is necessai y to exert a net force on it for some duration of time. The product of the force and the length of time it is applied is called the impulse and is the same as the change of momentum. Any increase in speed is directly projiortional to the impiulse and inversely proportional to its mass ... [Pg.965]

The ratio of rocket thrust to propellant mass flow, commonly called the specific impulse (/9p) of the propellant, represents a measure of the force developed per unit mass flow of propellant. From Eq. (2), it is apparent that high propellant-flame temperatures and low molecular-weight combustion products are required to produce high 7sp. [Pg.4]

The momentum of the mass flow into the front is zero, because the medium is initially at rest the momentum of the medium leaving the front with a velocity, u, is pQUudt, and this increase of momentum must equal the impulse of the net force per unit area of the front, that is of the difference in pressure in the shock and in the medium at rest, (p-pQ)dt. Thus ... [Pg.531]

In the above fig of a typical blast wave, peak pressure is the press increase at the shock front or the highest press in the wave minus atmospheric press, and is a measure of the max force exerted by the blast wave. Impulse is mathematically equal to rhe positive phase and is a measure of the force multiplied by the duration. The negative phase iasts considerably longer than the positive phase but the max negative press is only a fraction of the max positive press (See Ref 12,p 65ff)... [Pg.181]

After the pressure at the piston returns to zero, the gas is not acted upon by any external forces since the pressure in the cold gas is equal to zero both at x — —oo (in the limit at the boundary of dispersion), and at x — oo (x > X is sufficient) in the cold gas. In the motion, therefore, the total momentum of the gas, f pudx, is conserved. This momentum is equal to the pressure impulse of the piston,... [Pg.109]

For P increasing according to this law, in the limit, the impulse of the external force causing the motion (the impact impulse) I goes to zero I ss Pt ss t1/5. Consequently, the impulse equation for self-similar motion is written thus ... [Pg.110]

The central point within our consciousness, our "spirit" in the hermetic sense, can now be seen as an entity that can work to control quantum probabilities. To our "spirits" our brain is a quantum sea providing a rich realm in which it can incarnate and manifest patterns down into the electrical/chemical impulses of the nervous system. (It has been calculated that the number of interconnections existing in our brains far exceeds the number of atoms in the whole universe - so in this sense the microcosm truly mirrors the macrocosm ). Our "spirit" can through quantum borrowing momentarily press a certain order into this sea and this manifests as a thought, emotion, etc. Such an ordered state can only exist momentarily, before our spirit or point of consciousness is forced to jump and move to other regions of the brain, where at that moment the pattern of probability waves for the particles in these nerve cells, can reflect the form that our spirit is trying to work with. [Pg.8]

A second simulation focused on the roles of the forces on a generic atom in a melt caused by nonbonded interactions and those caused by the forces in its connecting bonds, and on the manner in which these forces varied with the reduced density p of the system Referring to Fig. 8a, let e and 2 be unit vectors directed along the bonds from fi to oq and oq, respectively. When [j is subjected to the impulsive / because of interaction through define... [Pg.20]

The determination of the thrust of a rocket motor involves recording the time diagram of the force (tons, kp, or newtons) during combustion. The force is allowed to act on a support, with a pick-up element thrust cell interposed between them. The measurement is carried out by the aid of a strain gauge element (variation of resistance with pressure) or of a piezo-quartz element, and the results are recorded on an oscillograph connected in a compensation circuit. Modern measuring and computation techniques yield the total thrust time (impulse) immediately. [Pg.400]

Therefore ve = u + Au -z and is the velocity of the ejected combustion gases relative to the rocket. Here the force (dm/df)ue corresponds to the thrust Fimpulse, which originates from the impulse of the system ... [Pg.60]

For Shaw the cause of the forces is infinitely great and beyond understanding. The philosopher can see how an impulse works its effect, but he does not know the working of the impulse itself. Nevertheless, it is extremely important to know that nothing would exist without the active principles. Shaw paraphrased Newton and argued ... [Pg.185]

A long memoir by Volta in two parts summarises his lecture to the Institut, repeats the above statements, and reports that by measuring the electrometer deflections with different pairs of metals he found that the forces which drive the electric fluid (alia forza. .. quelle spinge il fluido elettrico) from the first metal to the second are silver/copper i, copper/iron 2, iron/tin 3, lead/tin i, lead/zinc 5. Then the force for silver/zinc in immediate contact is 12 ( = i+ 2 + 3 + i+5), copper/tin 5 ( = 3 + 2), iron/zinc 9 (= 5 +1 + 3), etc. Thus the force or impulsion with which two metals act on the electric fluid is equal to the sum of the forces of the series of metals which stand between them, and... the electric force is the same as that which arises when the two extreme metals are in direct contact. Metals of any kind interposed between the two extreme metals have no effect on the force of the latter. This is the first statement of what Maxwell called Volta s law of contact electricity . Volta showed that it did not hold if humid conductors were in the circuit. E.g. HgO/Zn = I, hence if the law held HgO/Ag should be 13, but it was only i ( 25). The humid conductor reduces the electromotive force between the metals so that it is not balanced at the metallic junction, and a continuous current is kept up ( 7). In a summary of his publications Volta repeats his view that the current arises from the contact of two different conductors, above all metallic , and that the chemical action in the pile is not concerned with the production of electricity. [Pg.15]

Fig. 4 The parameter variations as a function of time under the impact of SW on a cylinder surrounded by a light gas layer (He the set of parameters conesponds to case 1 and Figs. 2 - 3) a) p t) at different points of the cylinder surface 1. .. 5 with 6 = 0, 45, 90, 135, 180 deg respectively (shock capturing algorithm and physical experiment) b) horizontal projection of the force C,(r) and the impulse I(t) striking a stationary cylinder (shock capturing algorithm). Fig. 4 The parameter variations as a function of time under the impact of SW on a cylinder surrounded by a light gas layer (He the set of parameters conesponds to case 1 and Figs. 2 - 3) a) p t) at different points of the cylinder surface 1. .. 5 with 6 = 0, 45, 90, 135, 180 deg respectively (shock capturing algorithm and physical experiment) b) horizontal projection of the force C,(r) and the impulse I(t) striking a stationary cylinder (shock capturing algorithm).

See other pages where Impulse of the force is mentioned: [Pg.1272]    [Pg.30]    [Pg.176]    [Pg.180]    [Pg.311]    [Pg.1582]    [Pg.1272]    [Pg.30]    [Pg.176]    [Pg.180]    [Pg.311]    [Pg.1582]    [Pg.318]    [Pg.322]    [Pg.325]    [Pg.91]    [Pg.25]    [Pg.44]    [Pg.369]    [Pg.260]    [Pg.1104]    [Pg.46]    [Pg.9]    [Pg.22]    [Pg.381]    [Pg.264]    [Pg.381]    [Pg.191]    [Pg.47]    [Pg.170]    [Pg.791]    [Pg.322]    [Pg.22]    [Pg.38]    [Pg.206]    [Pg.107]   
See also in sourсe #XX -- [ Pg.30 ]




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