1 |
jpye |
2785 |
#LyX 2.1 created this file. For more info see http://www.lyx.org/ |
2 |
|
|
\lyxformat 474 |
3 |
johnpye |
825 |
\begin_document |
4 |
|
|
\begin_header |
5 |
|
|
\textclass book |
6 |
jpye |
2785 |
\use_default_options false |
7 |
|
|
\maintain_unincluded_children false |
8 |
johnpye |
825 |
\language english |
9 |
jpye |
2785 |
\language_package default |
10 |
johnpye |
825 |
\inputencoding auto |
11 |
jpye |
2785 |
\fontencoding global |
12 |
|
|
\font_roman default |
13 |
|
|
\font_sans default |
14 |
|
|
\font_typewriter default |
15 |
|
|
\font_math auto |
16 |
|
|
\font_default_family default |
17 |
|
|
\use_non_tex_fonts false |
18 |
|
|
\font_sc false |
19 |
|
|
\font_osf false |
20 |
|
|
\font_sf_scale 100 |
21 |
|
|
\font_tt_scale 100 |
22 |
johnpye |
825 |
\graphics default |
23 |
jpye |
2785 |
\default_output_format default |
24 |
|
|
\output_sync 0 |
25 |
|
|
\bibtex_command default |
26 |
|
|
\index_command default |
27 |
johnpye |
825 |
\paperfontsize default |
28 |
|
|
\spacing single |
29 |
jpye |
2785 |
\use_hyperref false |
30 |
johnpye |
825 |
\papersize a4paper |
31 |
|
|
\use_geometry false |
32 |
jpye |
2785 |
\use_package amsmath 2 |
33 |
|
|
\use_package amssymb 2 |
34 |
|
|
\use_package cancel 1 |
35 |
|
|
\use_package esint 0 |
36 |
|
|
\use_package mathdots 0 |
37 |
|
|
\use_package mathtools 1 |
38 |
|
|
\use_package mhchem 0 |
39 |
|
|
\use_package stackrel 1 |
40 |
|
|
\use_package stmaryrd 1 |
41 |
|
|
\use_package undertilde 1 |
42 |
johnpye |
825 |
\cite_engine basic |
43 |
jpye |
2785 |
\cite_engine_type default |
44 |
|
|
\biblio_style plain |
45 |
johnpye |
825 |
\use_bibtopic false |
46 |
jpye |
2785 |
\use_indices false |
47 |
johnpye |
825 |
\paperorientation portrait |
48 |
jpye |
2785 |
\suppress_date false |
49 |
|
|
\justification true |
50 |
|
|
\use_refstyle 0 |
51 |
|
|
\index Index |
52 |
|
|
\shortcut idx |
53 |
|
|
\color #008000 |
54 |
|
|
\end_index |
55 |
johnpye |
825 |
\secnumdepth 3 |
56 |
|
|
\tocdepth 3 |
57 |
|
|
\paragraph_separation indent |
58 |
jpye |
2785 |
\paragraph_indentation default |
59 |
johnpye |
825 |
\quotes_language english |
60 |
|
|
\papercolumns 1 |
61 |
|
|
\papersides 2 |
62 |
|
|
\paperpagestyle default |
63 |
|
|
\tracking_changes false |
64 |
jpye |
2785 |
\output_changes false |
65 |
|
|
\html_math_output 0 |
66 |
|
|
\html_css_as_file 0 |
67 |
|
|
\html_be_strict false |
68 |
johnpye |
825 |
\end_header |
69 |
|
|
|
70 |
|
|
\begin_body |
71 |
|
|
|
72 |
|
|
\begin_layout Chapter |
73 |
|
|
Entering Dimensional Equations |
74 |
jpye |
2785 |
\begin_inset Index idx |
75 |
|
|
status collapsed |
76 |
johnpye |
825 |
|
77 |
jpye |
2785 |
\begin_layout Plain Layout |
78 |
|
|
equation, dimensional |
79 |
|
|
\end_layout |
80 |
|
|
|
81 |
johnpye |
825 |
\end_inset |
82 |
|
|
|
83 |
|
|
from Handbooks |
84 |
jpye |
2785 |
\begin_inset CommandInset label |
85 |
|
|
LatexCommand label |
86 |
|
|
name "cha:dimeqns" |
87 |
johnpye |
825 |
|
88 |
|
|
\end_inset |
89 |
|
|
|
90 |
|
|
|
91 |
|
|
\end_layout |
92 |
|
|
|
93 |
|
|
\begin_layout Standard |
94 |
|
|
Often in creating an ASCEND model one needs to enter a correlation |
95 |
jpye |
2785 |
\begin_inset Index idx |
96 |
|
|
status collapsed |
97 |
johnpye |
825 |
|
98 |
jpye |
2785 |
\begin_layout Plain Layout |
99 |
|
|
correlation |
100 |
|
|
\end_layout |
101 |
|
|
|
102 |
johnpye |
825 |
\end_inset |
103 |
|
|
|
104 |
|
|
given in a handbook that is written in terms of variables expressed in |
105 |
|
|
specific units. |
106 |
|
|
In this chapter, we examine how to do this easily and correctly in a system |
107 |
|
|
like ASCEND where all equations must be dimensionally correct. |
108 |
|
|
\end_layout |
109 |
|
|
|
110 |
|
|
\begin_layout Section |
111 |
|
|
Example 1-- vapor pressure |
112 |
jpye |
2785 |
\begin_inset Index idx |
113 |
|
|
status collapsed |
114 |
johnpye |
825 |
|
115 |
jpye |
2785 |
\begin_layout Plain Layout |
116 |
|
|
pressure, vapor |
117 |
|
|
\end_layout |
118 |
|
|
|
119 |
johnpye |
825 |
\end_inset |
120 |
|
|
|
121 |
|
|
|
122 |
|
|
\end_layout |
123 |
|
|
|
124 |
|
|
\begin_layout Standard |
125 |
|
|
Our first example is the equation to express vapor pressure using an Antoine |
126 |
jpye |
2785 |
\begin_inset Index idx |
127 |
|
|
status collapsed |
128 |
johnpye |
825 |
|
129 |
jpye |
2785 |
\begin_layout Plain Layout |
130 |
|
|
Antoine |
131 |
|
|
\end_layout |
132 |
|
|
|
133 |
johnpye |
825 |
\end_inset |
134 |
|
|
|
135 |
|
|
-like equation of the form: |
136 |
|
|
\end_layout |
137 |
|
|
|
138 |
|
|
\begin_layout Standard |
139 |
jpye |
2785 |
\begin_inset Formula |
140 |
|
|
\begin{equation} |
141 |
|
|
\ln(P_{sat})=A-\frac{B}{T+C}\label{eqn:dimeqns.lnPsat} |
142 |
|
|
\end{equation} |
143 |
johnpye |
825 |
|
144 |
|
|
\end_inset |
145 |
|
|
|
146 |
|
|
where |
147 |
|
|
\begin_inset Formula $P_{sat}$ |
148 |
|
|
\end_inset |
149 |
|
|
|
150 |
|
|
is in {atm} and |
151 |
|
|
\begin_inset Formula $T$ |
152 |
|
|
\end_inset |
153 |
|
|
|
154 |
|
|
in {R}. |
155 |
|
|
When one encounters this equation in a handbook, one then finds tabulated |
156 |
|
|
values for |
157 |
|
|
\begin_inset Formula $A$ |
158 |
|
|
\end_inset |
159 |
|
|
|
160 |
|
|
, |
161 |
|
|
\begin_inset Formula $B$ |
162 |
|
|
\end_inset |
163 |
|
|
|
164 |
|
|
and |
165 |
|
|
\begin_inset Formula $C$ |
166 |
|
|
\end_inset |
167 |
|
|
|
168 |
|
|
for different chemical species. |
169 |
|
|
The question we are addressing is: |
170 |
|
|
\end_layout |
171 |
|
|
|
172 |
|
|
\begin_layout Quote |
173 |
|
|
How should one enter this equation into ASCEND so one can then enter the |
174 |
|
|
constants A, B, and C with the exact values given in the handbook? |
175 |
|
|
\end_layout |
176 |
|
|
|
177 |
|
|
\begin_layout Standard |
178 |
|
|
ASCEND uses SI |
179 |
jpye |
2785 |
\begin_inset Index idx |
180 |
|
|
status collapsed |
181 |
johnpye |
825 |
|
182 |
jpye |
2785 |
\begin_layout Plain Layout |
183 |
|
|
SI |
184 |
|
|
\end_layout |
185 |
|
|
|
186 |
johnpye |
825 |
\end_inset |
187 |
|
|
|
188 |
|
|
units internally. |
189 |
|
|
Therefore, P would have the units {kg/m/s^2}, and T would have the units |
190 |
|
|
{K}. |
191 |
|
|
\end_layout |
192 |
|
|
|
193 |
|
|
\begin_layout Standard |
194 |
|
|
Eqn |
195 |
jpye |
2785 |
\begin_inset CommandInset ref |
196 |
|
|
LatexCommand ref |
197 |
|
|
reference "eqn:dimeqns.lnPsat" |
198 |
johnpye |
825 |
|
199 |
|
|
\end_inset |
200 |
|
|
|
201 |
|
|
|
202 |
|
|
\noun off |
203 |
|
|
is, in fact, dimensionally incorrect as written. |
204 |
|
|
We know how to use this equation, but ASCEND does not as ASCEND requires |
205 |
|
|
that we write dimensionally correct equations. |
206 |
|
|
For one thing, we can legitimately take the natural log (ln) only of unitless |
207 |
|
|
quantities. |
208 |
|
|
Also, the handbook will tabulate the values for A, B and C without units. |
209 |
|
|
If A is dimensionless, then B and C would require the dimensions of temperature. |
210 |
|
|
\end_layout |
211 |
|
|
|
212 |
|
|
\begin_layout Standard |
213 |
|
|
The mindset we describe in this chapter is to enter such equations is to |
214 |
|
|
make all quantities that must be expressed in particular units into dimensionle |
215 |
|
|
ss quantities that have the correct numerical value. |
216 |
|
|
\end_layout |
217 |
|
|
|
218 |
|
|
\begin_layout Standard |
219 |
|
|
We illustrate in the following subsections just how to do this conversion. |
220 |
|
|
It proves to be very straight forward to do. |
221 |
|
|
\end_layout |
222 |
|
|
|
223 |
|
|
\begin_layout Subsection |
224 |
|
|
Converting the ln term |
225 |
|
|
\end_layout |
226 |
|
|
|
227 |
|
|
\begin_layout Standard |
228 |
|
|
Convert the quantity within the ln() term into a dimensionless number that |
229 |
|
|
has the value of pressure when pressure is expressed in {atm}. |
230 |
|
|
\end_layout |
231 |
|
|
|
232 |
|
|
\begin_layout Standard |
233 |
|
|
Very simply, we write |
234 |
|
|
\end_layout |
235 |
|
|
|
236 |
|
|
\begin_layout LyX-Code |
237 |
|
|
P_atm = P/1{atm}; |
238 |
|
|
\end_layout |
239 |
|
|
|
240 |
|
|
\begin_layout Standard |
241 |
|
|
Note that P_atm has to be a dimensionless quantity here. |
242 |
|
|
\end_layout |
243 |
|
|
|
244 |
|
|
\begin_layout Standard |
245 |
|
|
We then rewrite the LHS of Equation |
246 |
jpye |
2785 |
\begin_inset CommandInset ref |
247 |
|
|
LatexCommand ref |
248 |
|
|
reference "eqn:dimeqns.lnPsat" |
249 |
johnpye |
825 |
|
250 |
|
|
\end_inset |
251 |
|
|
|
252 |
|
|
|
253 |
|
|
\noun off |
254 |
|
|
as |
255 |
|
|
\end_layout |
256 |
|
|
|
257 |
|
|
\begin_layout LyX-Code |
258 |
|
|
ln(P_atm) |
259 |
|
|
\end_layout |
260 |
|
|
|
261 |
|
|
\begin_layout Standard |
262 |
|
|
Suppose P = 2 {atm}. |
263 |
|
|
In SI units P= 202,650 {kg/m/s^2}. |
264 |
|
|
In SI units, the dimensional constant 1{atm} is about 101,325 {kg/m/s^2}. |
265 |
|
|
Using this definition, P_atm has the value 2 and is dimensionless. |
266 |
|
|
ASCEND will not complain with P_atm as the argument of the ln |
267 |
jpye |
2785 |
\begin_inset Index idx |
268 |
|
|
status collapsed |
269 |
johnpye |
825 |
|
270 |
jpye |
2785 |
\begin_layout Plain Layout |
271 |
|
|
ln |
272 |
|
|
\end_layout |
273 |
|
|
|
274 |
johnpye |
825 |
\end_inset |
275 |
|
|
|
276 |
|
|
() function, as it can take the natural log of the dimensionless |
277 |
jpye |
2785 |
\begin_inset Index idx |
278 |
|
|
status collapsed |
279 |
johnpye |
825 |
|
280 |
jpye |
2785 |
\begin_layout Plain Layout |
281 |
|
|
dimensionless |
282 |
|
|
\end_layout |
283 |
|
|
|
284 |
johnpye |
825 |
\end_inset |
285 |
|
|
|
286 |
|
|
quantity 2 without any difficulty. |
287 |
|
|
\end_layout |
288 |
|
|
|
289 |
|
|
\begin_layout Subsection |
290 |
|
|
Converting the RHS |
291 |
|
|
\end_layout |
292 |
|
|
|
293 |
|
|
\begin_layout Standard |
294 |
|
|
We next convert the RHS of Equation |
295 |
jpye |
2785 |
\begin_inset CommandInset ref |
296 |
|
|
LatexCommand ref |
297 |
|
|
reference "eqn:dimeqns.lnPsat" |
298 |
johnpye |
825 |
|
299 |
|
|
\end_inset |
300 |
|
|
|
301 |
|
|
|
302 |
|
|
\noun off |
303 |
|
|
, and it is equally as simple. |
304 |
|
|
Again, convert the temperature used in the RHS into: |
305 |
|
|
\end_layout |
306 |
|
|
|
307 |
|
|
\begin_layout LyX-Code |
308 |
|
|
T_R = T/1{R}; |
309 |
|
|
\end_layout |
310 |
|
|
|
311 |
|
|
\begin_layout Standard |
312 |
|
|
ASCEND converts the dimensional constant 1{R} into 0.55555555...{K}. |
313 |
|
|
Thus T_R is dimensionless but has the value that T would have if expressed |
314 |
|
|
in {R}. |
315 |
|
|
\end_layout |
316 |
|
|
|
317 |
|
|
\begin_layout Subsection |
318 |
|
|
In summary for example 1 |
319 |
|
|
\end_layout |
320 |
|
|
|
321 |
|
|
\begin_layout Standard |
322 |
|
|
We do not need to introduce the intermediate dimensionless variables. |
323 |
|
|
Rather we can write: |
324 |
|
|
\end_layout |
325 |
|
|
|
326 |
|
|
\begin_layout LyX-Code |
327 |
|
|
ln(P/1{atm}) = A - B/(T/1{R} + C); |
328 |
|
|
\end_layout |
329 |
|
|
|
330 |
|
|
\begin_layout Standard |
331 |
|
|
as a correct form for the dimensional equation. |
332 |
|
|
When we do it in this way, we can enter A, B and C as dimensionless quantities |
333 |
|
|
with the values exactly as tabulated. |
334 |
|
|
\end_layout |
335 |
|
|
|
336 |
|
|
\begin_layout Section |
337 |
|
|
Fahrenheit |
338 |
jpye |
2785 |
\begin_inset Index idx |
339 |
|
|
status collapsed |
340 |
johnpye |
825 |
|
341 |
jpye |
2785 |
\begin_layout Plain Layout |
342 |
|
|
Fahrenheit |
343 |
|
|
\end_layout |
344 |
|
|
|
345 |
johnpye |
825 |
\end_inset |
346 |
|
|
|
347 |
|
|
-- variables with offset |
348 |
jpye |
2785 |
\begin_inset CommandInset label |
349 |
|
|
LatexCommand label |
350 |
|
|
name "sec:dimeqns.Fahrenheit" |
351 |
johnpye |
825 |
|
352 |
|
|
\end_inset |
353 |
|
|
|
354 |
|
|
|
355 |
|
|
\end_layout |
356 |
|
|
|
357 |
|
|
\begin_layout Standard |
358 |
|
|
What if we write Equation |
359 |
jpye |
2785 |
\begin_inset CommandInset ref |
360 |
|
|
LatexCommand ref |
361 |
|
|
reference "eqn:dimeqns.lnPsat" |
362 |
johnpye |
825 |
|
363 |
|
|
\end_inset |
364 |
|
|
|
365 |
|
|
|
366 |
|
|
\noun off |
367 |
|
|
but the handbook says that T is in degrees Fahrenheit, i.e., in {F}? The |
368 |
|
|
conversion from {K} to {F} is |
369 |
|
|
\end_layout |
370 |
|
|
|
371 |
|
|
\begin_layout LyX-Code |
372 |
|
|
T{F} = T{K}*1.8 - 459.67 |
373 |
|
|
\end_layout |
374 |
|
|
|
375 |
|
|
\begin_layout Standard |
376 |
|
|
and the 459.67 is an offset. |
377 |
|
|
ASCEND does not support an offset for units conversion. |
378 |
|
|
We shall discuss the reasons for this apparent limitation in Section |
379 |
jpye |
2785 |
\begin_inset CommandInset ref |
380 |
|
|
LatexCommand ref |
381 |
|
|
reference "ssec:dimeqns.handlingUnitConv" |
382 |
johnpye |
825 |
|
383 |
|
|
\end_inset |
384 |
|
|
|
385 |
|
|
. |
386 |
|
|
\end_layout |
387 |
|
|
|
388 |
|
|
\begin_layout Standard |
389 |
|
|
You can readily handle temperatures in {F} if you again think as we did |
390 |
|
|
above. |
391 |
|
|
The rule, even for units requiring an offset for conversion, remains: convert |
392 |
|
|
a dimensional variable into dimensionless one such that the dimensionless |
393 |
|
|
one has the proper value. |
394 |
|
|
\end_layout |
395 |
|
|
|
396 |
|
|
\begin_layout Standard |
397 |
|
|
Define a new variable |
398 |
|
|
\end_layout |
399 |
|
|
|
400 |
|
|
\begin_layout LyX-Code |
401 |
|
|
T_degF = T/1{R} - 459.67; |
402 |
|
|
\end_layout |
403 |
|
|
|
404 |
|
|
\begin_layout Standard |
405 |
|
|
Then code |
406 |
jpye |
2785 |
\begin_inset CommandInset ref |
407 |
|
|
LatexCommand ref |
408 |
|
|
reference "eqn:dimeqns.lnPsat" |
409 |
johnpye |
825 |
|
410 |
|
|
\end_inset |
411 |
|
|
|
412 |
|
|
|
413 |
|
|
\noun on |
414 |
|
|
Equation 7.1 |
415 |
|
|
\noun off |
416 |
|
|
as |
417 |
|
|
\end_layout |
418 |
|
|
|
419 |
|
|
\begin_layout LyX-Code |
420 |
|
|
ln(P/1{atm}) = A - B/(T_degF + C); |
421 |
|
|
\end_layout |
422 |
|
|
|
423 |
|
|
\begin_layout Standard |
424 |
|
|
when entering it into ASCEND. |
425 |
|
|
You will then enter constants A, B, and C as dimensionless quantities having |
426 |
|
|
the values exactly as tabulated. |
427 |
|
|
In this example we must create the intermediate variable T_degF. |
428 |
|
|
\end_layout |
429 |
|
|
|
430 |
|
|
\begin_layout Section |
431 |
|
|
Example 3-- pressure drop |
432 |
jpye |
2785 |
\begin_inset CommandInset label |
433 |
|
|
LatexCommand label |
434 |
|
|
name "ssec:dimeqns.pressure drop" |
435 |
johnpye |
825 |
|
436 |
|
|
\end_inset |
437 |
|
|
|
438 |
|
|
|
439 |
|
|
\end_layout |
440 |
|
|
|
441 |
|
|
\begin_layout Standard |
442 |
|
|
From the Chemical Engineering Handbook |
443 |
jpye |
2785 |
\begin_inset Index idx |
444 |
|
|
status collapsed |
445 |
johnpye |
825 |
|
446 |
jpye |
2785 |
\begin_layout Plain Layout |
447 |
|
|
Chemical Engineering Handbook |
448 |
|
|
\end_layout |
449 |
|
|
|
450 |
johnpye |
825 |
\end_inset |
451 |
|
|
|
452 |
|
|
by Perry |
453 |
jpye |
2785 |
\begin_inset Index idx |
454 |
|
|
status collapsed |
455 |
johnpye |
825 |
|
456 |
jpye |
2785 |
\begin_layout Plain Layout |
457 |
|
|
Perry |
458 |
|
|
\end_layout |
459 |
|
|
|
460 |
johnpye |
825 |
\end_inset |
461 |
|
|
|
462 |
|
|
and Chilton |
463 |
jpye |
2785 |
\begin_inset Index idx |
464 |
|
|
status collapsed |
465 |
johnpye |
825 |
|
466 |
jpye |
2785 |
\begin_layout Plain Layout |
467 |
|
|
Chilton |
468 |
|
|
\end_layout |
469 |
|
|
|
470 |
johnpye |
825 |
\end_inset |
471 |
|
|
|
472 |
|
|
, Fifth Edition, McGraw-Hill, p10-33, we find the following correlation: |
473 |
|
|
\end_layout |
474 |
|
|
|
475 |
|
|
\begin_layout Standard |
476 |
jpye |
2785 |
\begin_inset Formula |
477 |
|
|
\[ |
478 |
|
|
\Delta P_{a}^{\prime}=\frac{y(V_{g}-V_{l})G^{2}}{144g} |
479 |
|
|
\] |
480 |
johnpye |
825 |
|
481 |
|
|
\end_inset |
482 |
|
|
|
483 |
|
|
where the pressure drop on the LHS is in psi, y is the fraction vapor by |
484 |
|
|
weight (i.e., dimensionless), Vg and Vl are the specific volumes of gas and |
485 |
|
|
liquid respectively in ft3/lbm, G is the mass velocity in lbm/hr/ft2 and |
486 |
|
|
g is the acceleration by gravity and equal to 4.18x108 ft/hr2. |
487 |
|
|
\end_layout |
488 |
|
|
|
489 |
|
|
\begin_layout Standard |
490 |
|
|
We proceed by making each term dimensionless and with the right numerical |
491 |
|
|
value for the units in which it is to be expressed. |
492 |
|
|
The following is the result. |
493 |
|
|
We do this by simply dividing each dimensional variable by the correct |
494 |
|
|
unit conversion factor. |
495 |
|
|
\end_layout |
496 |
|
|
|
497 |
|
|
\begin_layout LyX-Code |
498 |
|
|
delPa/1{psi} = y*(Vg-Vl)/1{ft^3/lbm}* |
499 |
|
|
\end_layout |
500 |
|
|
|
501 |
|
|
\begin_layout LyX-Code |
502 |
|
|
(G/1{lbm/hr/ft^2})^2/(144*4.18e8); |
503 |
|
|
\end_layout |
504 |
|
|
|
505 |
|
|
\begin_layout Section |
506 |
|
|
The difficulty of handling unit conversions defined with offset |
507 |
jpye |
2785 |
\begin_inset CommandInset label |
508 |
|
|
LatexCommand label |
509 |
|
|
name "ssec:dimeqns.handlingUnitConv" |
510 |
johnpye |
825 |
|
511 |
|
|
\end_inset |
512 |
|
|
|
513 |
|
|
|
514 |
|
|
\end_layout |
515 |
|
|
|
516 |
|
|
\begin_layout Standard |
517 |
|
|
How do you convert temperature from Kelvin to centigrade? The ASCEND compiler |
518 |
|
|
encounters the following ASCEND statement: |
519 |
|
|
\end_layout |
520 |
|
|
|
521 |
|
|
\begin_layout LyX-Code |
522 |
|
|
d1T1 = d1T2 + a.Td[4]; |
523 |
|
|
\end_layout |
524 |
|
|
|
525 |
|
|
\begin_layout Standard |
526 |
|
|
and d1T1 is supposed to be reported in centigrade. |
527 |
|
|
We know that ASCEND stores termperatures in Kelvin {K}. |
528 |
|
|
We also know that one converts {K} to {C} with the following relationshipT{C} |
529 |
|
|
= T{K} - 273.15. |
530 |
|
|
\end_layout |
531 |
|
|
|
532 |
|
|
\begin_layout Standard |
533 |
|
|
Now suppose d1T2 has the value 173.15 {K} and a.Td{4} has the value 500 {K}. |
534 |
|
|
What is d1T1 in {C}? It would appear to have the value 173.15+500-273.15 |
535 |
|
|
= 400 {C}. |
536 |
|
|
But what if the three variables here are really temperature differences? |
537 |
|
|
Then the conversion should be T{dC} = T{dK}, where we use the notation |
538 |
|
|
{dC} to be the units for temperature difference in centigrade and {dK} |
539 |
|
|
for differences in Kelvin. |
540 |
|
|
Then the correct answer is 173.15+500=673.15 {dC}. |
541 |
|
|
|
542 |
|
|
\end_layout |
543 |
|
|
|
544 |
|
|
\begin_layout Standard |
545 |
|
|
Suppose d1T1 is a temperature and d1T2 is a temperature difference (which |
546 |
|
|
would indicate an unfortunate but allowable naming scheme by the creator |
547 |
|
|
of this statement). |
548 |
|
|
It turns out that a.Td[4] is then required to be a temperature and not a |
549 |
|
|
temperature difference for this equation to make sense. |
550 |
|
|
We discover that an equation written to have a right-hand-side of zero |
551 |
|
|
and that involves the sums and differences of temperature and temperature |
552 |
|
|
difference variables will have to have an equal number of positive and |
553 |
|
|
negative temperatures in it to make sense, with the remaining having to |
554 |
|
|
be temperature differences. |
555 |
|
|
Of course if the equation is a correlation, such may not be the case, as |
556 |
|
|
the person deriving the correlation is free to create an equation that |
557 |
|
|
"fits" the data without requiring the equation to be dimensionally (and |
558 |
|
|
physically) reasonable. |
559 |
|
|
\end_layout |
560 |
|
|
|
561 |
|
|
\begin_layout Standard |
562 |
|
|
We could create the above discussion just as easily in terms of pressure |
563 |
|
|
where we distinguish absolute from gauge pressures (e.g., {psia} vs. |
564 |
|
|
{psig}). |
565 |
|
|
We would find the need to introduce units {dpisa} and {dpsig} also. |
566 |
|
|
|
567 |
|
|
\end_layout |
568 |
|
|
|
569 |
|
|
\begin_layout Subsection |
570 |
|
|
General offset |
571 |
jpye |
2785 |
\begin_inset Index idx |
572 |
|
|
status collapsed |
573 |
johnpye |
825 |
|
574 |
jpye |
2785 |
\begin_layout Plain Layout |
575 |
|
|
offset |
576 |
|
|
\end_layout |
577 |
|
|
|
578 |
johnpye |
825 |
\end_inset |
579 |
|
|
|
580 |
|
|
and difference units |
581 |
jpye |
2785 |
\begin_inset Index idx |
582 |
|
|
status collapsed |
583 |
johnpye |
825 |
|
584 |
jpye |
2785 |
\begin_layout Plain Layout |
585 |
|
|
difference units |
586 |
|
|
\end_layout |
587 |
|
|
|
588 |
johnpye |
825 |
\end_inset |
589 |
|
|
|
590 |
|
|
|
591 |
|
|
\end_layout |
592 |
|
|
|
593 |
|
|
\begin_layout Standard |
594 |
|
|
Unfortunately, we find we have to think much more generally than the above. |
595 |
|
|
Any unit conversion can be introduced both with and without offset. |
596 |
|
|
Suppose we have an equation which involves the sums and diffences of terms |
597 |
|
|
t1 to t4: |
598 |
|
|
\end_layout |
599 |
|
|
|
600 |
|
|
\begin_layout Standard |
601 |
jpye |
2785 |
\begin_inset Formula |
602 |
|
|
\begin{equation} |
603 |
|
|
t_{1}+t_{2}-(t+t_{4})=0\label{eqn:t1+t2} |
604 |
|
|
\end{equation} |
605 |
johnpye |
825 |
|
606 |
|
|
\end_inset |
607 |
|
|
|
608 |
|
|
where the units for each term is some combination of basic units, e.g., {ft/s^2/R}. |
609 |
|
|
Let us call this combination {X} and add it to our set of allowable units, |
610 |
|
|
i.e., we define |
611 |
|
|
\emph on |
612 |
|
|
{X} = {ft/s^2/R}. |
613 |
|
|
|
614 |
|
|
\emph default |
615 |
|
|
|
616 |
|
|
\end_layout |
617 |
|
|
|
618 |
|
|
\begin_layout Standard |
619 |
|
|
Suppose we define units {Xoffset} to satisfy: {Xoffset} = {X} - 10 as another |
620 |
|
|
set of units for our system. |
621 |
|
|
We will also have to introduce the concept of {dX} and and should probably |
622 |
|
|
introduce also {dXoffset} to our system, with these two obeying{dXoffset} |
623 |
|
|
= {Xoffset}. |
624 |
|
|
|
625 |
|
|
\end_layout |
626 |
|
|
|
627 |
|
|
\begin_layout Standard |
628 |
|
|
For what we might call a "well-posed" equation, we can argue that the coefficien |
629 |
|
|
t of variables in units such as {Xoffset} have to add to zero with the remaining |
630 |
|
|
being in units of {dX} and {dXoffset}. |
631 |
|
|
Unfortunately, the authors of correlation equations are not forced to follow |
632 |
|
|
any such rule, so you can find many published correlations that make the |
633 |
|
|
most awful (and often unstated) assumptions about the units of the variables |
634 |
|
|
being correlated. |
635 |
|
|
\end_layout |
636 |
|
|
|
637 |
|
|
\begin_layout Standard |
638 |
|
|
Will the typical modeler get this right? We suspect not. |
639 |
|
|
We would need a very large number of unit conversion combinations in both |
640 |
|
|
absolute, offset and relative units to accomodate this approach. |
641 |
|
|
\end_layout |
642 |
|
|
|
643 |
|
|
\begin_layout Standard |
644 |
|
|
We suggest that our approach to use only absolute units with no offset is |
645 |
|
|
the least confusing for a user. |
646 |
|
|
Units conversion is then just multiplication by a factor both for absolute |
647 |
|
|
{X} and difference {dX} units-- we do not have to introduce difference |
648 |
|
|
variables because we do not introduce offset units. |
649 |
|
|
|
650 |
|
|
\end_layout |
651 |
|
|
|
652 |
|
|
\begin_layout Standard |
653 |
|
|
When users want offset units such as gauge pressure or Fahrenheit for temperatur |
654 |
|
|
e, they can use the conversion to dimensionless variables having the right |
655 |
|
|
value, using the style we introduced above, i.e., T_defF = T/1{R} - 459.67 |
656 |
|
|
and P_psig = P/1{psi} - 14.696 as needed. |
657 |
|
|
\end_layout |
658 |
|
|
|
659 |
|
|
\begin_layout Standard |
660 |
|
|
Both approaches to handling offset introduce undesirable and desirable character |
661 |
|
|
istics to a modeling system. |
662 |
|
|
Neither allow the user to use units without thinking carefully. |
663 |
|
|
We voted for this form because of its much lower complexity. |
664 |
|
|
\end_layout |
665 |
|
|
|
666 |
|
|
\end_body |
667 |
|
|
\end_document |