-
Notifications
You must be signed in to change notification settings - Fork 0
Expand file tree
/
Copy pathApplicationsOfIntegration.Rmd
More file actions
1070 lines (632 loc) · 20.3 KB
/
Copy pathApplicationsOfIntegration.Rmd
File metadata and controls
1070 lines (632 loc) · 20.3 KB
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
208
209
210
211
212
213
214
215
216
217
218
219
220
221
222
223
224
225
226
227
228
229
230
231
232
233
234
235
236
237
238
239
240
241
242
243
244
245
246
247
248
249
250
251
252
253
254
255
256
257
258
259
260
261
262
263
264
265
266
267
268
269
270
271
272
273
274
275
276
277
278
279
280
281
282
283
284
285
286
287
288
289
290
291
292
293
294
295
296
297
298
299
300
301
302
303
304
305
306
307
308
309
310
311
312
313
314
315
316
317
318
319
320
321
322
323
324
325
326
327
328
329
330
331
332
333
334
335
336
337
338
339
340
341
342
343
344
345
346
347
348
349
350
351
352
353
354
355
356
357
358
359
360
361
362
363
364
365
366
367
368
369
370
371
372
373
374
375
376
377
378
379
380
381
382
383
384
385
386
387
388
389
390
391
392
393
394
395
396
397
398
399
400
401
402
403
404
405
406
407
408
409
410
411
412
413
414
415
416
417
418
419
420
421
422
423
424
425
426
427
428
429
430
431
432
433
434
435
436
437
438
439
440
441
442
443
444
445
446
447
448
449
450
451
452
453
454
455
456
457
458
459
460
461
462
463
464
465
466
467
468
469
470
471
472
473
474
475
476
477
478
479
480
481
482
483
484
485
486
487
488
489
490
491
492
493
494
495
496
497
498
499
500
501
502
503
504
505
506
507
508
509
510
511
512
513
514
515
516
517
518
519
520
521
522
523
524
525
526
527
528
529
530
531
532
533
534
535
536
537
538
539
540
541
542
543
544
545
546
547
548
549
550
551
552
553
554
555
556
557
558
559
560
561
562
563
564
565
566
567
568
569
570
571
572
573
574
575
576
577
578
579
580
581
582
583
584
585
586
587
588
589
590
591
592
593
594
595
596
597
598
599
600
601
602
603
604
605
606
607
608
609
610
611
612
613
614
615
616
617
618
619
620
621
622
623
624
625
626
627
628
629
630
631
632
633
634
635
636
637
638
639
640
641
642
643
644
645
646
647
648
649
650
651
652
653
654
655
656
657
658
659
660
661
662
663
664
665
666
667
668
669
670
671
672
673
674
675
676
677
678
679
680
681
682
683
684
685
686
687
688
689
690
691
692
693
694
695
696
697
698
699
700
701
702
703
704
705
706
707
708
709
710
711
712
713
714
715
716
717
718
719
720
721
722
723
724
725
726
727
728
729
730
731
732
733
734
735
736
737
738
739
740
741
742
743
744
745
746
747
748
749
750
751
752
753
754
755
756
757
758
759
760
761
762
763
764
765
766
767
768
769
770
771
772
773
774
775
776
777
778
779
780
781
782
783
784
785
786
787
788
789
790
791
792
793
794
795
796
797
798
799
800
801
802
803
804
805
806
807
808
809
810
811
812
813
814
815
816
817
818
819
820
821
822
823
824
825
826
827
828
829
830
831
832
833
834
835
836
837
838
839
840
841
842
843
844
845
846
847
848
849
850
851
852
853
854
855
856
857
858
859
860
861
862
863
864
865
866
867
868
869
870
871
872
873
874
875
876
877
878
879
880
881
882
883
884
885
886
887
888
889
890
891
892
893
894
895
896
897
898
899
900
901
902
903
904
905
906
907
908
909
910
911
912
913
914
915
916
917
918
919
920
921
922
923
924
925
926
927
928
929
930
931
932
933
934
935
936
937
938
939
940
941
942
943
944
945
946
947
948
949
950
951
952
953
954
955
956
957
958
959
960
961
962
963
964
965
966
967
968
969
970
971
972
973
974
975
976
977
978
979
980
981
982
983
984
985
986
987
988
989
990
991
992
993
994
995
996
997
998
999
1000
# Applications of Integration
## Areas Between Curves
In single-variable calculus, we first learn to compute the area under a curve using definite integrals. This idea naturally extends to finding the area between two curves. Instead of measuring the distance from a function to the \(x\)-axis, we now measure the vertical distance between two functions across an interval.
Suppose two continuous functions \( f(x) \) and \( g(x) \) are defined on an interval \([a,b]\), and assume
\[
f(x) \ge g(x) \quad \text{for all } x \in [a,b].
\]
At each point \(x\), the vertical distance between the curves is
\[
f(x) - g(x).
\]
By summing these vertical distances over the interval using rectangles and taking a limit, we define the area between the curves as a definite integral.
<div class="theorem">
Area Formula (Vertical Slices)
If \( f(x) \ge g(x) \) on \([a,b]\), then the area \(A\) between the curves is
\[
A = \int_a^b \big(f(x) - g(x)\big)\,dx.
\]
</div>
**Interpretation:**
- **Top curve:** \( y_T = f(x) \)
- **Bottom curve:** \( y_B = g(x) \)
- **Rectangle height:** \( y_T - y_B \)
- **Rectangle width:** \( dx \)
So each rectangle has area
\[
(y_T - y_B)\,dx,
\]
and the integral adds all such rectangles across the interval.
**Geometric Meaning:**
This formula generalizes area under a curve:
- If \( g(x)=0 \), then the formula reduces to
\[
A = \int_a^b f(x)\,dx,
\]
which is exactly the area under \(y=f(x)\).
Thus, **area between curves = area under top curve − area under bottom curve**.
::: {.example}
Simple Polynomial Curves
Find the area between \( y = x^2 \) and \( y = x \) on \([0,1]\).
**Solution:**
**Step 1: Identify top and bottom curves**
On \(0 \le x \le 1\),
\[
x \ge x^2 \Rightarrow y_T = x,\; y_B = x^2.
\]
**Step 2: Set up the integral**
\[
A = \int_0^1 (x - x^2)\,dx.
\]
**Step 3: Evaluate**
\[
A = \int_0^1 x\,dx - \int_0^1 x^2\,dx
= \left[\frac{x^2}{2}\right]_0^1 - \left[\frac{x^3}{3}\right]_0^1
= \frac{1}{2} - \frac{1}{3}
= \frac{1}{6}.
\]
Therefore,
\[
A = \frac{1}{6}.
\]
:::
::: {.example}
Exponential and Linear Functions
Find the area between \( y = e^x \) and \( y = x \) on \([0,1]\).
**Solution:**
**Top curve:** \( e^x \)
**Bottom curve:** \( x \)
\[
A = \int_0^1 (e^x - x)\,dx
\]
\[
A = \left[e^x - \frac{x^2}{2}\right]_0^1
= \left(e - \frac{1}{2}\right) - (1 - 0)
= e - \frac{3}{2}.
\]
Therefore,
\[
A = e - \frac{3}{2}.
\]
:::
::: {.example}
Intersection Points First
Find the area enclosed by \( y = x^2 \) and \( y = 2x - x^2 \).
**Solution:**
**Step 1: Find intersections**
\[
x^2 = 2x - x^2 \Rightarrow 2x^2 - 2x = 0 \Rightarrow 2x(x-1)=0
\]
\[
x=0,\; x=1
\]
**Step 2: Identify top and bottom**
\[
y_T = 2x - x^2,\quad y_B = x^2
\]
**Step 3: Set up integral**
\[
A = \int_0^1 \big[(2x - x^2) - x^2\big]\,dx
= \int_0^1 (2x - 2x^2)\,dx
\]
**Step 4: Evaluate**
\[
A = 2\int_0^1 (x - x^2)\,dx
= 2\left(\frac{1}{2} - \frac{1}{3}\right)
= 2\cdot \frac{1}{6}
= \frac{1}{3}.
\]
Therefore,
\[
A = \frac{1}{3}.
\]
:::
---
### When Curves Cross (Absolute Value Form)
If the curves switch which one is on top, the area must be computed using
\[
A = \int_a^b |f(x) - g(x)|\,dx,
\]
which is evaluated by **splitting the interval at intersection points** and computing each region separately.
---
### Horizontal Slices (Integrating with Respect to \(y\))
Sometimes regions are easier to describe using horizontal rectangles.
If the region is bounded by
\[
x = x_R(y), \quad x = x_L(y), \quad y \in [c,d],
\]
then
\[
A = \int_c^d \big(x_R(y) - x_L(y)\big)\,dy.
\]
This is especially useful when:
- the curves are sideways parabolas,
- the region has complicated vertical boundaries,
- vertical slicing would require splitting into multiple integrals.
---
### Putting It All Together
> **Core principle:**
> Area between curves = accumulation of distance between boundaries.
- Area is computed by **integrating vertical or horizontal distances** between curves.
- Every area problem follows the same structure:
1. Identify the region.
2. Determine intersection points.
3. Identify top/bottom or left/right curves.
4. Subtract functions correctly.
5. Integrate over the correct limits.
**Vertical slicing:**
\[
A = \int_a^b \big(y_T - y_B\big)\,dx
\]
**Horizontal slicing:**
\[
A = \int_c^d \big(x_R - x_L\big)\,dy
\]
---
#### Conceptual Takeaways
- Area is **accumulated distance**, not just height.
- Integration converts geometry into algebra.
- Choosing the correct slicing direction (vertical vs horizontal) simplifies computation.
- Graphing the region is not optional — it is part of the solution method.
- Absolute value represents **total geometric area**, not signed area.
---
#### Skills You Should Be Able To Do
After mastering this section, you should be able to:
- Sketch regions between curves
- Find intersection points algebraically or numerically
- Identify top/bottom and left/right boundaries
- Set up correct definite integrals for area
- Use both \(dx\) and \(dy\) formulations
- Split integrals when curves cross
- Interpret area in applied contexts (physics, biology, economics)
- Translate geometry into integral expressions
---
#### Problems
## Volumes
Just as calculus provides a precise definition of **area** using limits and integrals, it also provides a precise definition of **volume**. While we have an intuitive sense of what volume means, calculus allows us to compute exact volumes for complex solids by breaking them into thin slices and adding their volumes.
We begin with simple solids like cylinders, where the volume formula is already known. From there, we generalize the idea by slicing more complicated solids into thin slabs, approximating each slab by a cylinder, and using limits to obtain an exact result.
---
### Volume of a Cylinder
A **right cylinder** is formed by two congruent, parallel bases separated by a fixed height \(h\). If the base has area \(A\), then the volume is
\[
V = A h.
\]
- Circular cylinder (radius \(r\)):
\[
V = \pi r^2 h
\]
- Rectangular box (length \(l\), width \(w\), height \(h\)):
\[
V = lwh
\]
These formulas are special cases of a more general integral definition of volume.
---
### Cross-Sections and Slicing
To compute the volume of a general solid:
1. Slice the solid with planes.
2. Each slice produces a **cross-section**.
3. Approximate each slice by a thin cylinder.
4. Add all slices using integration.
Let \(A(x)\) be the area of the cross-section at position \(x\). If the solid lies between \(x=a\) and \(x=b\), then its volume is defined by
\[
V = \int_a^b A(x)\,dx.
\]
**Interpretation**
- Each slice has volume \( A(x)\,dx \)
- The integral adds all these slices
- Volume = accumulation of cross-sectional areas
<div class="theorem">
Fundamental Volume Formula
**Vertical slicing:**
\[
V = \int_a^b A(x)\,dx
\]
**Horizontal slicing:**
\[
V = \int_c^d A(y)\,dy
\]
</div>
::: {.example}
Volume of a Sphere
Find the volume of a sphere of radius \(r\).
**Solution:**
At position \(x\), the cross-section is a circle with radius
\[
y = \sqrt{r^2 - x^2}.
\]
So the area is
\[
A(x) = \pi y^2 = \pi(r^2 - x^2).
\]
**Integral**
\[
V = \int_{-r}^{r} \pi(r^2 - x^2)\,dx
\]
**Evaluation**
\begin{align*}
V &= \pi \int_{-r}^{r} (r^2 - x^2)\,dx\\
&= \pi \left[ r^2 x - \frac{x^3}{3} \right]_{-r}^{r}\\
&= \frac{4}{3}\pi r^3.
\end{align*}
Therefore,
\[
V = \frac{4}{3}\pi r^3.
\]
:::
::: {.example}
Solid of Revolution (Disk Method)
Rotate \(y=\sqrt{x}\) from \(x=0\) to \(x=1\) about the \(x\)-axis.
**Solution:**
The cross-sections are disks with radius \( \sqrt{x} \).
\[
A(x) = \pi(\sqrt{x})^2 = \pi x
\]
\begin{align*}
V &= \int_0^1 \pi x\,dx\\
&= \pi \left[\frac{x^2}{2}\right]_0^1\\
&= \frac{\pi}{2}.
\end{align*}
Therefore,
\[
V = \frac{\pi}{2}.
\]
:::
::: {.example}
Washer Method
Rotate the region between \(y=x\) and \(y=x^2\) on \([0,1]\) about the \(x\)-axis.
**Solution:**
- Outer radius: \(R=x\)
- Inner radius: \(r=x^2\)
\[
A(x) = \pi(R^2 - r^2) = \pi(x^2 - x^4)
\]
\begin{align*}
V &= \int_0^1 \pi(x^2 - x^4)\,dx\\
&= \pi\left[\frac{x^3}{3} - \frac{x^5}{5}\right]_0^1\\
&= \pi\left(\frac{1}{3}-\frac{1}{5}\right)\\
&= \frac{2\pi}{15}.
\end{align*}
Therefore,
\[
V = \frac{2\pi}{15}.
\]
:::
---
### Solids of Revolution
<div class="definition">
A **solid of revolution** is formed by rotating a region about a line.
**Disk Method**
\[
A = \pi r^2
\]
**Washer Method**
\[
A = \pi(R^2 - r^2)
\]
**Volume Formula**
\[
V = \int A\,dx \quad \text{or} \quad V = \int A\,dy.
\]
</div>
---
### Pulling It All Together
> Volume is accumulated cross-sectional area.
Every volume problem follows the same structure:
1. Identify the slicing direction
2. Determine the cross-section shape
3. Express its area as a function
4. Integrate over the correct limits
> **Core principle:**
> Geometry defines the cross-section.
> Calculus accumulates it.
> Integration creates volume.
---
#### Conceptual Takeaways
- Volume is defined through **limits and accumulation**
- Slicing turns 3D geometry into 1D integration
- Geometry determines the algebra
- Choosing the right slicing direction simplifies the problem
- All volume formulas come from the same integral principle
- Disks, washers, and general cross-sections are just special cases of \(V=\int A\)
---
#### Skills You Should Be Able To Do
After this section, you should be able to:
- Interpret volume as accumulated area
- Identify appropriate cross-sections
- Choose between vertical and horizontal slicing
- Set up volume integrals correctly
- Use disk and washer methods
- Compute volumes of solids of revolution
- Compute volumes of non-revolution solids
- Translate geometry into area functions
- Sketch solids and cross-sections
- Model real-world volume problems mathematically
---
#### Problems
## Volumes by Cylindrical Shells
Some volume problems become algebraically difficult when using the **disk** or **washer** methods, especially when the region must be solved for \( x \) in terms of \( y \) (or vice versa). In many cases, this leads to complicated equations that are hard to invert or integrate.
The **method of cylindrical shells** provides an alternative approach that often avoids these difficulties. Instead of slicing the region perpendicular to the axis of rotation, we slice it parallel to the axis of rotation. When these slices are rotated, they form **thin cylindrical shells**.
This method is especially useful when:
- Solving for one variable is algebraically difficult
- Washer radii are complicated functions
- The region is more naturally described using vertical or horizontal strips
A typical cylindrical shell has:
- **Radius**: distance from the axis of rotation to the slice
- **Circumference**: \( 2\pi(\text{radius}) \)
- **Height**: length of the slice (given by the function or difference of functions)
- **Thickness**: \( dx \) or \( dy \)
The volume of a single shell is given by:
\[
V_{\text{shell}} \;\approx\; (\text{circumference})(\text{height})(\text{thickness})
\]
\[
V_{\text{shell}} \;\approx\; 2\pi r \, h \, \Delta x
\]
<div class="theorem">
Shell Method Formula
**Rotation about the y-axis using vertical slices**
If a region under \( y = f(x) \) from \( x=a \) to \( x=b \) is rotated about the y-axis:
\[
V \;=\; \int_a^b 2\pi x\, f(x)\, dx,
\]
where:
- radius \( = x \)
- height \( = f(x) \)
- thickness \( = dx \)
**Rotation about the x-axis using horizontal slices**
\[
V \;=\; \int_c^d 2\pi y\, (\text{horizontal length})\, dy
\]
where:
- radius \( = y \)
- height = horizontal length of region
- thickness \( = dy \)
</div>
::: {.example}
Rotation about the y-axis
Find the volume of the solid obtained by rotating the region bounded by
\[
y = 2x^2 - x^3 \quad \text{and} \quad y = 0
\]
about the **y-axis**.
**Solution:**
Using cylindrical shells:
- radius: \( x \)
- height: \( 2x^2 - x^3 \)
- thickness: \( dx \)
\begin{align*}
V &= \int_0^2 2\pi x(2x^2 - x^3)\, dx\\
& = 2\pi \int_0^2 (2x^3 - x^4)\, dx\\
& = 2\pi \left[ \frac{1}{2}x^4 - \frac{1}{5}x^5 \right]_0^2\\
& = 2\pi \left( 8 - \frac{32}{5} \right) \\
& = \frac{16\pi}{5}.
\end{align*}
:::
::: {.example}
Region Between Two Curves
Rotate the region between \( y = x \) and \( y = x^2 \) about the y-axis.
**Solution:**
- radius: \( x \)
- height: \( x - x^2 \)
\begin{align*}
V &= \int_0^1 2\pi x(x - x^2)\, dx\\
& = 2\pi \int_0^1 (x^2 - x^3)\, dx\\
& = 2\pi \left[ \frac{x^3}{3} - \frac{x^4}{4} \right]_0^1\\
& = 2\pi\left(\frac{1}{3} - \frac{1}{4}\right)\\
& = \frac{\pi}{6}.
\end{align*}
:::
::: {.example}
Rotation about the x-axis
Rotate the region under \( y=\sqrt{x} \) from \( x=0 \) to \( x=1 \) about the **x-axis**.
**Solution:**
Rewrite as:
\[
x = y^2
\]
Using shells (horizontal slices):
- radius: \( y \)
- height: \( 1 - y^2 \)
\begin{align*}
V &= \int_0^1 2\pi y(1 - y^2)\, dy\\
&= 2\pi \int_0^1 (y - y^3)\, dy\\
&= 2\pi \left[ \frac{y^2}{2} - \frac{y^4}{4} \right]_0^1\\
&= 2\pi\left(\frac{1}{2} - \frac{1}{4}\right)\\
&= \frac{\pi}{2}.
\end{align*}
:::
Shells also work when rotating about lines like \( x=c \).
**General Pattern:**
- radius = distance from slice to line of rotation
- circumference = \( 2\pi(\text{radius}) \)
- height = top − bottom of region
---
### Pulling It All Together
**When Shells Are Better Than Washers**
Use shells when:
- Solving for \( x \) in terms of \( y \) is difficult
- Washer radii require complicated algebra
- Region is naturally described with vertical or horizontal strips
- One method gives one integral instead of two
- One variable leads to simpler bounds
\[
V = \int (\text{circumference})(\text{height})(\text{thickness})
\]
\[
V = \int 2\pi(\text{radius})(\text{height})\, d(\text{variable})
\]
#### Conceptual Takeaways
The shell method works by:
- slicing **parallel** to the axis of rotation
- rotating each slice into a **cylindrical shell**
- adding up volumes using integration
Instead of finding cross-sectional areas (disks/washers), we use **surface geometry**:
> circumference × height × thickness
This geometric viewpoint makes many problems algebraically simpler and conceptually clearer.
---
#### Skills You Should Be Able To Do
After this section, you should be able to:
- Identify when the shell method is preferable to disks/washers
- Sketch the region and axis of rotation
- Determine:
- shell radius
- shell height
- correct thickness variable
- Set up shell integrals correctly
- Choose correct bounds of integration
- Handle rotations about:
- x-axis
- y-axis
- vertical lines \( x=c \)
- horizontal lines \( y=c \)
- Compare shell vs washer methods
- Translate geometry into integrals
- Interpret volume using geometric reasoning
---
#### Problems
## Work
---
#### Problems
## Average Value of a Function
Finding the average of finitely many numbers is straightforward:
\[
y_{\text{avg}} = \frac{y_1 + y_2 + \cdots + y_n}{n}
\]
But many real-world quantities vary continuously:
- temperature over a day
- velocity during a trip
- power usage over time
- density across a region
In these cases, there are infinitely many values, so we use integration to define an average value for a function over an interval.
<div class="note">
**Deriving the Average Value Formula**
Let \( y = f(x) \) be defined on an interval \( [a,b] \).
1. Divide the interval into \( n \) subintervals of width:
\[
\Delta x = \frac{b-a}{n}
\]
2. Choose a sample point \( x_i^* \) in each subinterval.
3. Average the function values:
\[
\frac{f(x_1^*) + f(x_2^*) + \cdots + f(x_n^*)}{n}
\]
Rewriting using \( \Delta x \) and taking the limit as \( n \to \infty \):
\[
f_{\text{avg}} = \frac{1}{b-a}\int_a^b f(x)\,dx
\]
</div>
**Average Value Formula**
\[
f_{\text{avg}} = \frac{1}{b-a}\int_a^b f(x)\,dx.
\]
**Geometric Interpretation**
For **positive functions**:
\[
\frac{\text{Area under curve}}{\text{Width of interval}} = \text{Average height}
\]
This means the average value is the **height of a rectangle** over \( [a,b] \) that has the **same area** as the region under \( f(x) \).
::: {.example}
Computing an Average Value
Find the average value of
\[
f(x) = 1 + x^2
\]
on the interval \( [-1,2] \).
**Solution:**
\begin{align*}
f_{\text{avg}} &= \frac{1}{2 - (-1)}\int_{-1}^{2} (1 + x^2)\,dx\\
& = \frac{1}{3}\int_{-1}^{2} (1 + x^2)\,dx\\
& = \frac{1}{3}\left[ x + \frac{x^3}{3} \right]_{-1}^{2}\\
& = \frac{1}{3}\Big[(2 + \tfrac{8}{3}) - (-1 - \tfrac{1}{3})\Big]\\
& = \frac{1}{3}(6)\\
& = 2.
\end{align*}
:::
---
### Mean Value Theorem for Integrals
<div class="definition">
**MVT for Integrals**
If \( f \) is **continuous** on \( [a,b] \), then there exists at least one number
\( c \in [a,b] \) such that:
\[
f(c) = f_{\text{avg}} = \frac{1}{b-a}\int_a^b f(x)\,dx.
\]
Equivalently:
\[
\int_a^b f(x)\,dx = f(c)(b-a).
\]
</div>
Geometrically, there exists a point \( c \) where the function’s height equals the average height over the interval.
> This means: a rectangle of height \( f(c) \) and base \( [a,b] \) has the same area as the area under the curve.
::: {.example}
Finding the Mean Value Point
Using the previous example, we found:
\[
f_{\text{avg}} = 2
\]
Solve:
\[
f(c) = 2
\]
\[
1 + c^2 = 2
\]
\[
c^2 = 1
\]
\[
c = \pm 1
\]
Both \( c=-1 \) and \( c=1 \) lie in the interval \( [-1,2] \), so both satisfy the theorem.
</div>
---
### Application: Average Velocity
Let \( s(t) \) be position and \( v(t) = s'(t) \) be velocity.
**Average velocity (definition):**
\[
v_{\text{avg}} = \frac{s(t_2) - s(t_1)}{t_2 - t_1}
\]
**Average value of velocity function:**
\[
v_{\text{avg}} = \frac{1}{t_2 - t_1}\int_{t_1}^{t_2} v(t)\,dt
\]
Using the Net Change Theorem:
\[
\int_{t_1}^{t_2} v(t)\,dt = s(t_2) - s(t_1)
\]
So:
\[
\text{Average velocity} = \text{Average value of velocity function}
\]
This shows that **physical average velocity** and **integral-based average value** are mathematically identical.
---
### Pulling It All Together
Think:
> **Average value = total accumulation ÷ interval length**
or
> **Area ÷ width = average height**
\[
f_{\text{avg}} = \frac{1}{b-a}\int_a^b f(x)\,dx