05.04.2016 Views

Modern Engineering Thermodynamics

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

736 CHAPTER 18: Introduction to Statistical <strong>Thermodynamics</strong><br />

Substituting Eq. (18.19) into Eq. (18.23) and carrying out the integration gives<br />

where<br />

NðV 1 ! V 2 Þ<br />

N<br />

= erfðx 2 Þ − erfðx 1 Þ − p 2 ffiffiffi ðx 2 e −x2 2 − x1 e −x2 1 Þ (18.24)<br />

π<br />

pffiffiffi<br />

Z x<br />

x 1 = V 1 /V mp , x 2 = V 2 /V mp , and erfðxÞ = error function of x = 2/ π e − x2 dx<br />

Representative values for the error function can be found in Table 18.2. Note that erf(0) = 0 and erf(∞) = 1.<br />

0<br />

3<br />

V mp = 395 m/s<br />

f(V) ×1000<br />

2<br />

1<br />

V avg = 445 m/s<br />

V rms = 483 m/s<br />

0 0 100 200 300 400 500 600 700 800 900 1000<br />

Velocity (m/s)<br />

FIGURE 18.5<br />

The Maxwell velocity distribution function f(V ) for oxygen (O 2 ) at 300 K as defined by Eq. (18.19).<br />

Table 18.2 Values of the Error Function<br />

x<br />

erf(x)<br />

0.0 0.0<br />

0.1 0.1125<br />

0.2 0.2227<br />

0.3 0.3286<br />

0.4 0.4284<br />

0.5 0.5205<br />

0.6 0.6039<br />

0.7 0.6778<br />

0.8 0.7421<br />

0.9 0.7969<br />

1.0 0.8427<br />

1.2 0.9103<br />

1.4 0.9523<br />

1.6 0.9764<br />

1.8 0.9891<br />

2.0 0.9953<br />

2.2 0.9981<br />

2.4 0.9993<br />

2.6 0.9998<br />

2.8 0.9999<br />

∞ 1.0<br />

<br />

<br />

Note: For all x, erfðxÞ = p 2 ffiffi π<br />

x − x3<br />

3ð1!Þ + x5<br />

5ð2!Þ − x7<br />

7ð3!Þ + … , and exp − x 2 = 1 − x 2 /1! + x 4 /2! − x 6 /3! + x 8 /4! − …

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!