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Modern Engineering Thermodynamics

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50 CHAPTER 2: Thermodynamic Concepts<br />

EXAMPLE 2.4 (Continued )<br />

Solution<br />

From Eq. (2.19), we compute the muzzle velocity as<br />

<br />

V projectile = 1 + m <br />

<br />

pendulum<br />

½2gRð1 − cos⁡yÞŠ 1/2 = 1 + 5:0kg <br />

½29:81 ð m/s 2 Þð1:5mÞð1 − cos 15° ÞŠ 1/2<br />

m projectile<br />

0:01 kg<br />

= 5:0 × 10 2 m/s<br />

Exercises<br />

6. To bring down large game requires at least 2500. ft·lbf of impact energy (the impact energy of a high-speed projectile is<br />

its kinetic energy on impact). Determine the necessary impact velocity for the following projectiles (recall that there are<br />

7000 grains in 1 lbm): (a) a 200. grain bullet, (b) 300. grain bullet, and (c) a 500. grain bullet. Answers: (a) 2370 ft/s,<br />

(b) 1940. ft/s, (c) 1500 ft/s.<br />

7. Determine the displacement angle produced when a 0.3125 lbm baseball traveling at 90.0 miles per hour is “caught” by<br />

a ballistic pendulum having a 3.00 ft support cable and a mass of 180. lbm. Answer: 1.33°.<br />

2.12 CONSERVATION OF MASS<br />

An important application of the balance equation is to one of the basic conserved physical quantities, mass.<br />

Since mass is conserved in all nonnuclear reactions, its net production in any system is zero. Therefore,<br />

Eq. (2.10) tells us that the mass balance equation has the form<br />

<br />

<br />

<br />

Net gain in mass by the Net mass transported into<br />

= (2.20)<br />

system during time dt the system during time dt<br />

This statement can be cast in mathematical form via Eq. (2.11) as m G = m T (since m P = 0),andEq.(2.12)<br />

provides the rate form of this balance equation as _m G = _m T (since _m P = 0). In more precise mathematical<br />

language, the mass balance (MB) measured over some time interval δt can be written as<br />

Mass balance ðMBÞ over time δt = ðδmÞ system<br />

= ∑m in −∑m out (2.21)<br />

and the mass rate balance (MRB) becomes<br />

<br />

Mass rate balance ðMRBÞ = dm <br />

dt<br />

system<br />

= ∑ _m in −∑ _m out (2.22)<br />

One of the most common uses of the conservation of mass balance equation is in chemistry. Chemical reaction<br />

equations are simply mass balances. Though reaction equations are not usually written as equalities, the left-hand<br />

side is the total mass of reactants used and the right-hand side is the total mass of products produced by the reaction.<br />

Since mass is conserved in chemical reactions, these two masses must be equal. For example, the reaction<br />

indicated by the equation A + B = C + D means that the mass of A plus the mass of B is the same as the mass of C<br />

plus the mass of D. These equations are valid either for individual molecules or groups of molecules that bear the<br />

same reaction relation as the individual molecules. These molecular groups, called moles, form the macroscopic<br />

basis for chemistry and chemical engineering. This concept is illustrated in the following example.<br />

EXAMPLE 2.5<br />

The total mass of a system is conserved in a chemical reaction, but the mass of any particular chemical species is not necessarily<br />

conserved. Show that the following chemical reaction is just a closed system mass balance for the chemical species<br />

involved:<br />

n a A + n b B ! n c C + n d D<br />

where A, B, C, and D are the chemical species, and n a , n b , n c , and n d are their molar amounts.<br />

Solution<br />

When a chemical reaction occurs in a closed system, the mass transport term vanishes and then a mass balance for a chemical<br />

species X becomes “the mass of X gained in the reaction must equal the mass of X produced by the reaction and this must equal the

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