Solutions to the 2003 AP Calculus AB Exam (Form B)

Louis A. Talman
Department of Mathematical & Computer Sciences
Metropolitan State College of Denver

•Problem 1.

•a.

If f[x] = 4 x^2 - x^3, and g[x] = 18 - 3 x, then the curves have an intersection in the first quadrant where x = 3.

In[1]:=

Solve[4 x^2 - x^3 == 18 - 3 x, x]

Out[1]=

{{x -> -2}, {x -> 3}, {x -> 3}}

We have f '[x] = 8 x - 3 x^2, so the equation of the line tangent to the curve y = f[x] at x = 3 is y = f[3] + f '[3] (x - 3),
or y = (4 · 3^2 - 3^3) + (8 · 3 - 3 · 3^2) (x - 3) = 9 + (24 - 27) (x - 3).  This is y = 9 - 3 x + 9, or y = 18 - 3 x.

•b.

The curve y = f[x] intersects the x-axis at x = 4, and the line crosses the x-axis at x = 6.  Therefore the area of the region S is

In[2]:=

∫ _ 3^4 ((18 - 3 x) - (4 x^2 - x^3)) d x + ∫ _ 4^6 (18 - 3 x) d x

Out[2]=

95/12

•c.

The curve y = 4 x^2 - x^3 crosses the x-axis at x = 0 and at x = 4.  Thus, the volume generated when the region R is revolved about the x-axis is

In[3]:=

π ∫ _ 0^4 (4 x^2 - x^3)^2 d x

Out[3]=

(16384 π)/105

(Note:  I mistakenly found the area generated by the region S instead of the region R in an earlier version of these solutions.  Thanks to Heather Kelly for alerting me to the mistake.)

•Problem 2

In[4]:=

H[t_] = 2 + 10/(1 + Log[t + 1])

Out[4]=

2 + 10/(1 + Log[1 + t])

In[5]:=

R[t_] = 12 Sin[t^2/47]

Out[5]=

12 Sin[t^2/47]

•a.

The amount pumped into the tank during FormBox[RowBox[{0,  , <=, t, <=, RowBox[{12, Cell[]}]}], TraditionalForm] is given by ∫ _ 0^12 H[t] d t.  Integrating numerically, we obtain

In[6]:=

NIntegrate[H[t], {t, 0, 12}] gallons

Out[6]=

70.57085927390095` gallons

•b.

The rate of change of the volume of oil in the tank at time t is H[t] - R[t].  At t = 6 this is

In[7]:=

H[6.0] - R[6.0]

Out[7]=

-2.9241917345474207`

The level of oil in the tank is decreasing when t = 6 because the volume of oil in the tank has negative rate of change then.

•c.

We are given that there were 125 gallons of oil in the tank when t = 0.  Thus, the volume in the tank at time t is, by the Fundamental Theorem of Calculus, V[t] = 125 + ∫ _ 0^t (H[τ] - R[τ]) d τ.  Integrating numerically with t = 12, we obtain

In[8]:=

(125 + NIntegrate[H[τ] - R[τ], {τ, 0, 12}]) gallons

Out[8]=

122.02571305628209` gallons

•d.

Here is a plot of the rate at which the volume of oil in the tank changes.

In[9]:=

Plot[H[t] - R[t], {t, 0, 12}]

[Graphics:HTMLFiles/index_53.gif]

Out[9]=

-Graphics -

This rate is positive, and the volume increases, from t = 0 until about t = 5. The rate is negative, and the volume decreases, from about t = 5 until a little after t = 11.  Thereafter, volume increases.  This means that there is a minimum somewhere near t = 11.  Solving numerically, we locate the relevant critical point:

In[10]:=

t /. FindRoot[H[t] - R[t] == 0, {t, 11.0}][[1]]

Out[10]=

11.31847025145638`

The amount of oil in the tank is minimal when t = 11.3185.

•Problem 3.

•a.

Average radius is 1/720 ∫ _ 0^360 B[x] d x.

•b.

The required midpoint Riemann sum is

In[11]:=

1/720 (30 (120 - 0) + 30 (240 - 120) + 24 (360 - 240))

Out[11]=

14

•c.

The integral π ∫ _ 125^275 (B[x]/2)^2 d x gives the volume, in cubic millimeters, of the segment of the blood vessel that extends from x = 125mm to x = 275 mm.

•d.

We have B[60] = B[180].  Consequently, by Rolle's Theorem, there is a number x _ 1 ∈ (60, 180) where B '[x _ 1] = 0.  We also have B[240] = B[360], so, once again by Rolle's Theorem, there is a number x _ 2 ∈ (240, 360) where B '[x _ 2] = 0.  But then B '[x _ 1] = B '[x _ 2], so, yet again by Rolle's Theorem, there must be a number x _ 3 between x _ 1 and x _ 2, such that B ''[x _ 3] = 0.  Noting that 0 < x _ 1 < x _ 2 < 360, we see that x _ 3 ∈ (0, 360).

•Problem 4

•a.

If v[t] = -1 + e^(1 - t), then acceleration is a[t] = -e^(1 - t).  When t = 3, we have a[3] = -e^(-2).

•b.

Speed is S[t] = | v[t] |, and so S '[t] = v[t]/(| v[t] |) v '[t] = (-1 + e^(1 - t))/(| -1 + e^(1 - t) |) (-e^(1 - t)).  When t = 3, this is (-1 + e^(-2))/(1 - e^(-2)) (-e^(-2)), which is positive.  Hence S[t] is increasing when t = 3, because its derivative is positive there.

•c.

The particle changes direction where derivative of position with respect to time, which is velocity, changes sign.  This happens only when -1 + e^(1 - t) = 0, or when t = 1.

•d.

The total distance traveled (as opposed to the total displacement) by the particle over the interval 0 <= t <= 3 is ∫ _ 0^3 | v[t] | d t.  Taking into account the sign change at t = 1, this is ∫ _ 0^1 (e^(1 - t) - 1) d t + ∫ _ 1^3 (1 - e^(1 - t)) d t = (-e^(1 - t) - t) | _ 0^1 + (t + e^(1 - t)) | _ 1^3.  This reduces to e - 1 + 1/e^2.

•Problem 5

•a.

g[3] is the area of a rectangle of base 1 and height 2 plus the area of a triangle of base 1 and height 2, or  2 + 1 = 3.   By the Fundamental Theorem of Calculus, g '[x] = f[x], and when x = 3, this is f[3] = 2.  In the interval (2, 4), the FTC tells us that FormBox[RowBox[{g '[x],  , =,  , RowBox[{f[x],  , =,  , RowBox[{8,  , -,  , RowBox[{2,  , x, Cell[]}]}]}]}], TraditionalForm].  Thus g ''[x] = -2 in that interval, and g ''[3] = -2.

•b.

The average rate of change of g on [0, 3] is 1/3 ∫ _ 0^3 g '[x] d x = 1/3 (g[3] - g[0]) = 1/3 ( 3 - (-4)) = 7/3.  (See part a for the calculation of g[3]; for g[0], we have g[0] = ∫ _ 2^0 f[t] d t, which is the negative of the area of a triangle of base 2 and height 4, or -4.)

•c.

By the Fundamental Theorem of Calculus, g '[x] = f[x].  Thus, on the interval (0, 3), g '[x] takes on its average value, 7/3, at two different points:  x = 7/6, and x = 17/6 .

•d.

An inflection point occurs where the monotonicity of the derivative changes from increasing to decreasing or vice versa.  There are two such points for g '[x] = f[x], (We know g '[x] = f[x] by the Fundamental Theorem of Calculus.)  They are x = 2 and x = 5.

•Problem 6

•a.

If f '[x] = x f[x]^(1/2), then f ''[x] = f[x]^(1/2) + x/(2 f[x]^(1/2)) f '[x] = f[x] ^(1/2) + x/(2 f[x]^(1/2)) x f[x]^(1/2) = f[x]^(1/2) + x^2/2.  Thus, f ''[3] = 25^(1/2) + 9/2 = 19/2 .

•b.

We have f '[x]/f[x]^(1/2) = x, so, ∫ _ 3^x f '[s]/f[s]^(1/2) d s = ∫ _ 3^x s d s = 1/2 (x^2 - 9).  Substituting y = f[s], d y = f '[s] d s in the integral on the left, we transform it to ∫ _ 25^f[x] d y/y^(1/2) = 2 f[x]^(1/2) - 10.  Thus 2 f[x]^(1/2) - 10 = 1/2 (x^2 - 9), or FormBox[RowBox[{f[x]^(1/2), =, RowBox[{1/4 (x^2 - 9) + 5,  , =,  , RowBox[{1/4, RowBox[{(, RowBox[{x^2, +, RowBox[{11, Cell[]}]}], )}]}]}]}], TraditionalForm].  So f[x] = 1/16 (x^2 + 11)^2.


Converted by Mathematica  (May 14, 2003)