When you finish this section, you should be able to:
In this section, we discuss the Fundamental Theorem of Calculus, a method for finding integrals more easily, avoiding the need to find the limit of Riemann sums. The Fundamental Theorem is aptly named because it links the two branches of calculus: differential calculus and integral calculus. As it turns out, the Fundamental Theorem of Calculus has two parts, each of which relates an integral to an antiderivative.
Suppose \(f\) is a function that is continuous on a closed interval \([a,b]\). Then the definite integral \(\int_{a}^{b}f(x) \,dx\) exists and is equal to a real number. Now if \(x\) denotes any number in \([a,b] \), the definite integral \(\int_{a}^{x} {f(t)}\,dt\) exists and depends on \(x.\) That is, \({\int_{a}^{x} {f(t)}}\,dt\) is a function of \(x\), which we name \(I,\) for “integral.” \[ I(x)={\int_{a}^{x} {f(t)}}\,dt \]
Antiderivatives are discussed in Section 4.8, pp. xx-xx.
The domain of \(I\) is the closed interval \([a,b]\). The integral that defines \(I\) has a variable upper limit of integration \(x.\) The \(t\) that appears in the integrand is a dummy variable. Surprisingly, when we differentiate \(I\) with respect to \(x,\) we get back the original function \(f\). That is, \(\int_{a}^{x}f(t) \,dt\) is an antiderivative of \(f.\)
Let \(f\) be a function that is continuous on a closed interval \([a,b]\). The function \(I\) defined by \[ \boxed{\bbox[5pt]{ I\,(x)=\int_{a}^{x}f(t)\,dt } } \]
has the properties that it is continuous on \([a,b] \) and differentiable on \((a,b).\) Moreover, \[ \boxed{\bbox[5pt]{ I' (x)=\dfrac{d}{dx}\left[\int_{a}^{x}f(t)\,dt \right] =f(x) } } \]
for all \(x\) in \((a,b).\)
The proof of Part 1 of the Fundamental Theorem of Calculus is given in Appendix B. However, if the integral \(\int_{a}^{x}f(t)\, dt\) represents area, we can interpret the theorem using geometry.
Figure 22 shows the graph of a function \(f\) that is nonnegative and continuous on a closed interval \([a,b] .\) Then \(I(x) =\int_{a}^{x}f(t)\, dt\) equals the area under the graph of \(f\) from \(a\) to \(x.\)
\[ \begin{eqnarray} I(x) =\int_{a}^{x}f(t) \,dt &=& \hbox{the area under the graph of } f \hbox{ from } a \hbox{ to } x \nonumber \\ I(x+h) =\int_{a}^{x+h}f(t) \,dt &=& \hbox{the area under the graph of } f \hbox{ from } a \hbox{ to } x+h \nonumber\\ I(x+h) -I(x) &=& \hbox{the area under the graph of } f \hbox{ from } x \hbox{ to } x+h \nonumber\\ \dfrac{I(x+h) -I(x)}{h} &=& \dfrac{\hbox{the area under the graph of }f \hbox{ from } x \hbox{ to } x+h} {h}\qquad \end{eqnarray} \]
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Based on the definition of a derivative, \[ \begin{equation} \ \lim\limits_{h\rightarrow 0}\left[ \dfrac{I(x+h) -I(x) }{h}\right] =I^\prime (x) \end{equation} \]
Since \(f\) is continuous, \(\lim\limits_{h\rightarrow 0}f(x+h) =f(x) .\) As \(h\rightarrow 0,\) the area under the graph of \(f\) from \(x\) to \(x+h\) gets closer to the area of a rectangle with width \(h\) and height \(f(x)\). That is, \[ \begin{equation} \lim\limits_{h\rightarrow 0}\dfrac{\hbox{the area under the graph of }f \hbox{ from }x\hbox{ to }x+h}{h}=\lim\limits_{h\rightarrow 0}\dfrac{h[ f(x) ] }{h}=f(x) \end{equation} \]
Combining (1), (2), and (3), it follows that \(I^\prime (x) =f(x).\)
(a) \(\dfrac{d}{dx}\int_{0}^{x}\sqrt{t+1}\,dt=\sqrt{ x+1}\)
(b) \(\dfrac{d}{dx}\int_{2}^{x}\dfrac{s^{3}-1}{2s^{2}+s+1}ds=\dfrac{x^{3}-1}{2x^{2}+x+1}\)
Problem 5.
Find \(\dfrac{d}{dx}\int_{4}^{3x^{2}+1}\sqrt{e^{t}+t}\,dt\).
The Chain Rule is discussed in Section 3.1, pp. xx-xx.
Solution The upper limit of integration is a function of \(x\), so we use the Chain Rule along with Part 1 of the Fundamental Theorem of Calculus.
Let \(y=\int_{4}^{3x^{2}+1}\sqrt{e^{t}+t}\,dt\) and \(u(x) =3x^{2}+1.\) Then \(y=\int_{4}^{u}\sqrt{e^{t}+t}\,dt\) and \[ \begin{eqnarray*} \dfrac{d}{dx}\int_{4}^{3x^{2}+1}\sqrt{e^{t}+t}\,dt &=& \dfrac{dy}{dx} \underset{\underset{{\color{#0066A7}{\hbox{Chain Rule}}}}{\color{#0066A7}{\uparrow}}}{=} \dfrac{dy}{du}\cdot \dfrac{du}{dx}= \left[ \dfrac{d}{du}\int_{4}^{u}\sqrt{e^{t}+t}\,dt\right] \cdot \dfrac{du}{dx} \\ & \underset{\underset{\color{#0066A7}{{\hbox{Use the Fundamental Theorem}}}} {\color{#0066A7}{\uparrow}}}{=}& \sqrt{e^{u}+u}\cdot \dfrac{du}{dx} \underset{\underset{{\color{#0066A7}{{\hbox{\({u=3x}^{2}+1\); \(\dfrac{du}{dx}=6x\)}}}}{\hbox{\( \)}}}{\color{#0066A7}{\uparrow}}}{=}\sqrt{e^{( 3x^{2}+1) }+3x^{2}+1}\cdot 6x \\ \end{eqnarray*} \]
Problem 11.
Find \(\dfrac{d}{dx}\int_{x^{3}}^{5}(t^{4}+1)^{1/3}\,dt\).
Solution To use Part 1 of the Fundamental Theorem of Calculus, the variable must be part of the upper limit of integration. So, we use the fact that \(\int_{a}^{b}f(x)\,dx=-\int_{b}^{a}f(x)\,dx\) to interchange the limits of integration. \[ \dfrac{d}{dx}\int_{x^{3}}^{5}(t^{4}+1)^{1/3}\,dt=\dfrac{d}{dx}\left[ {-} \int_{5}^{x^{3}}(t^{4}+1)^{1/3} dt\right] ={-}\dfrac{d}{dx} \int_{5}^{x^{3}}(t^{4}+1)^{1/3} dt \]
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Now we use the Chain Rule. We let \(y=\int_{5}^{x^{3}}( t^{4}+1)^{1/3}dt\) and \(u(x) =x^{3}.\)
In these examples, the differentiation is with respect to the variable that appears in the upper or lower limit of integration and the answer is a function of that variable.
\[ \begin{eqnarray*} \dfrac{d}{dx}\int_{x^{3}}^{5}(t^{4}+1)^{1/3}\,dt &=& -\dfrac{d}{dx}\int_{5}^{x^{3}}(t^{4}+1)^{1/3}\,dt=-\dfrac{dy}{dx} \underset{ \underset{ \color{#0066A7}{\hbox{Chain Rule}} } {\color{#0066A7}{\uparrow}} } {=} -\dfrac{dy}{du}\cdot\dfrac{du}{dx}\\ &=&-\dfrac{d}{du}\int_{5}^{u}( t^{4}+1) ^{1/3}dt\cdot \dfrac{du}{dx} \\ &=& -(u^{4}+1)^{1/3}\cdot \dfrac{du}{dx} {\color{#0066A7}\enspace{\color{#0066A7}{\hbox{Use the Fundamental Theorem}}}} \\ &=&-( x^{12}+1) ^{1/3}\cdot 3x^{2} \enspace{\color{#0066A7}{{\hbox{\({u=x}^{3}\); \(\dfrac{du}{dx}=3x^{2}\)}}}} \\ &=&-3x^{2}(x^{12}+1)^{1/3} \end{eqnarray*} \]
Problem 15.
Part 1 of the Fundamental Theorem of Calculus establishes a relationship between the derivative and the definite integral. Part 2 of the Fundamental Theorem of Calculus provides a method for finding a definite integral without using Riemann sums.
Let \(f\) be a function that is continuous on a closed interval \([a,b]\). If \(F\) is any antiderivative of \(f\) on \([a,b]\), then \[ \boxed{\bbox[5pt]{ \int_{a}^{b}f(x)\,dx=F(b)-F(a)}} \]
Let \(I(x) =\int_{a}^{x}f(t)\, dt.\) Then from Part 1 of the Fundamental Theorem of Calculus, \(I=I(x) \) is continuous for \(a\leq x\leq b\) and differentiable for \(a\lt x\lt b\). So, \[ \dfrac{d}{dx}\int_{a}^{x}f(t) ~dt=f(x) \qquad a\lt x\lt b \]
Any two antiderivatives of a function differ by a constant.
That is, \(\int_{a}^{x}f(t)\,dt\) is an antiderivative of \(f\). So, if \(F\) is any antiderivative of \(f\), then \[ F(x)=\int_{a}^{x}f(t)\,dt+C \]
where \(C\) is some constant. Since \(F\) is continuous on \([a,b] ,\) we have
For any constant \(C\), \([F(b)+C]-[F(a)+C]=F(b)-F(a).\) In other words, it does not matter which antiderivative of \(f\) is chosen when using Part 2 of the Fundamental Theorem of Calculus, since the same answer is obtained for every antiderivative.
\[ F(a)=\int_{a}^{a}f(t) dt+C \qquad F(b)=\int_{a}^{b}f(t) dt+C \]
Since, \({\int_{a}^{a}{f(t) dt}=0}\), subtracting \(F(a)\) from \(F(b)\) gives \[ F(b)-F(a)=\int_{a}^{b}f(t) dt \]
Since \(t\) is a dummy variable, we can replace \(t\) by \(x\) and the result follows.
As an aid in computation, we introduce the notation \[ \boxed{\bbox[#FAF8ED,5pt]{ \int_{a}^{b}f(x)~dx= \Big[F(x)\Big] _{a}^{b}=F(b)-F(a)}} \]
The notation \(\big[F(x)\big] _{a}^{b}\) also suggests that to find \(\int_{a}^{b}f(x) \,dx,\) we first find an antiderivative \(F(x)\) of \(f(x)\). Then we write \(\big[F(x)\big]_{a}^{b}\) to represent \(F(b)-F(a)\).
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Use Part 2 of the Fundamental Theorem of Calculus to find:
Solution (a) An antiderivative of \(f(x) =x^{2}\) is \(F(x) =\dfrac{x^{3}}{3}\). By Part 2 of the Fundamental Theorem of Calculus, \[ {\int_{-2}^{1}{x^{2}}}dx=\left[ {\dfrac{{x^{3}}}{{3}}}\right] _{-2}^{1}={\dfrac{{1}^{3}}{{3}}}-{\dfrac{{\left( {-2}\right) ^{3}}}{{3}}}={\dfrac{{1}}{{3}}}+{\dfrac{{8}}{{3}}}={\dfrac{{9}}{{3}}}=3 \]
(b) An antiderivative of \(f(x) =\cos x\) is \(F(x) =\sin x\). By Part 2 of the Fundamental Theorem of Calculus, \[ \int_{0}^{\pi /6}\cos x\,dx= \Big[\sin x\Big] _{0}^{\pi /6}=\sin \dfrac{\pi }{6}-\sin 0=\dfrac{1}{2} \]
(c) An antiderivative of \(f(x) =\)\(\dfrac{1}{\sqrt{1-x^{2}}}\) is \(F(x) =\sin ^{-1}x\), provided \(\vert x\vert \lt1\). By Part 2 of the Fundamental Theorem of Calculus, \[ {\int_{0}^{\sqrt{3}/2}} \dfrac{1}{\sqrt{1-x^{2}}}\,dx= \Big[\sin^{-1}x\Big] _{0}^{\sqrt{3}/2}=\sin ^{-1}\dfrac{\sqrt{3}}{2}-\sin ^{-1}0=\dfrac{\pi}{3}-0=\dfrac{\pi}{3} \]
(d) An antiderivative of \(f(x)=\dfrac{1}{x}\) is \(F(x) =\ln \,\vert x\vert \). By Part 2 of the Fundamental Theorem of Calculus, \[ {\int_{1}^{2}} \dfrac{1}{x}\,dx= \Big[\ln \vert x\vert\Big] _{1}^{2}=\ln 2-\ln 1=\ln 2-0=\ln 2 \]
Problems 25 and 31.
Find the area under the graph of \(f(x) =e^{x}\) from \(-1\) to \(1.\)
Solution Figure 23 shows the graph of \(f(x)=e^{x}\) on the closed interval \([-1,1] \).
The area \(A\) under the graph of \(f\) from \(-1\) to \(1\) is given by \[ A= \int\nolimits_{-1}^{1}e^{x}\, dx=\Big[e^{x}\Big] _{-1}^{1}=e^{1}-e^{-1} = e-\dfrac{1}{e} \approx 2.35. \]
Problem 45.
Part 2 of the Fundamental Theorem of Calculus states that, under certain conditions, \[ \int_{a}^{b}f(x)\, dx=F(b) -F(a)\qquad \hbox{where } F^\prime =f \]
That is, \[ \int_{a}^{b} F^\prime (x)\, dx=F(b) -F(a) \]
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In other words, \[ \boxed{\bbox[#FAF8ED,5pt]{ \begin{array}{@{\hspace*{-4pt}}lll} &&\hbox{The integral from } a \hbox{ to } b \hbox{ of the rate of change of } F \hbox{ equals the change} \\ &&\hbox{ in } F \hbox{ from } a \hbox{ to } b. \end{array}}} \]
This interpretation of an integral is important since it reveals how to go from a rate of change of a function \(F\) back to the change itself.
Problem 51.