Problem 28
Question
Integrate \(f\) over the given region. Curved region \(f(s, t)=e^{s}\) Int over the region in the first quadrant of the st-plane that lies above the curve \(s=\ln t\) from \(t=1\) to \(t=2\)
Step-by-Step Solution
Verified Answer
The integral diverges to infinity.
1Step 1: Understanding the Region of Integration
The region of integration is in the first quadrant and is bounded from below by the curve \(s = \ln t\) and from the left by \(t=1\). The region extends from \(t=1\) to \(t=2\). Thus, for a fixed \(t\), \(s\) ranges from \(\ln t\) to some upper limit. Since there is no explicit upper bound for \(s\), we conclude it extends upwards to infinity.
2Step 2: Setting up the Integral
Based on the region of integration described, we set up the double integral. We first integrate with respect to \(s\) from \(s = \ln t\) to \(s = \infty\). Then, we integrate with respect to \(t\) from \(t = 1\) to \(t = 2\). This gives the integral \(\int_{1}^{2} \int_{\ln t}^{\infty} e^{s} \, ds \, dt.\)
3Step 3: Solving the Inner Integral
The inner integral \(\int_{\ln t}^{\infty} e^{s} \, ds\) involves integrating \(e^{s}\) from \(s = \ln t\) to infinity. The antiderivative of \(e^{s}\) is \(e^{s}\), so we have\[\int_{\ln t}^{\infty} e^{s} \, ds = \lim_{A \to \infty} [e^{s}]_{\ln t}^{A} = \lim_{A \to \infty} (e^{A} - e^{\ln t}).\]This simplifies to \(\lim_{A \to \infty} e^{A} - t = \infty - t\).
4Step 4: Evaluating the Outer Integral
The outer integral becomes \(\int_{1}^{2} (\infty - t) \, dt\). The term \(\infty - t\) clearly represents an improper integral that diverges to infinity, as \(\int_{1}^{2} \infty \, dt\) goes to infinity. Thus, no finite value can be assigned to this integral.
5Step 5: Concluding the Integration
The integral diverges. Since one of the bounds of integration extends to infinity and involves an expression that grows without bound, the entire definite integral does not converge to a finite, real number.
Key Concepts
Improper IntegralsRegion of IntegrationLimits of Integration
Improper Integrals
When dealing with improper integrals, it's crucial to recognize that one or more limits of integration are infinite or if the integrand exhibits discontinuities over the interval of integration. In our exercise, the inner integral is improper due to the upper limit of integration being infinity:
\[ \int_{\ln t}^{\infty} e^{s} \, ds. \]
Improper integrals are calculated by taking limits, allowing us to handle terms that involve infinity in a controlled way. For instance, when integrating the exponential function \(e^s\) from \(s = \ln t\) to infinity, we take the limit:
\[ \lim_{A \to \infty} [e^{s}]_{\ln t}^{A} = \lim_{A \to \infty} (e^{A} - e^{\ln t}) = \infty - t. \]
Recognizing the divergence, or non-convergence, is key when evaluating improper integrals. Here, the expression grows without bound, thus making the integral diverge and yield an infinite result.
\[ \int_{\ln t}^{\infty} e^{s} \, ds. \]
Improper integrals are calculated by taking limits, allowing us to handle terms that involve infinity in a controlled way. For instance, when integrating the exponential function \(e^s\) from \(s = \ln t\) to infinity, we take the limit:
\[ \lim_{A \to \infty} [e^{s}]_{\ln t}^{A} = \lim_{A \to \infty} (e^{A} - e^{\ln t}) = \infty - t. \]
Recognizing the divergence, or non-convergence, is key when evaluating improper integrals. Here, the expression grows without bound, thus making the integral diverge and yield an infinite result.
- Improper integrals occur with infinite limits.
- Handling improper integrals often involves evaluating limits.
- Divergence indicates the integral does not settle to a finite answer.
Region of Integration
Understanding the region of integration provides clarity for setting up integrals properly. In this problem, the region is outlined in the first quadrant on the \(st\)-plane. It's given by:
By visualizing the region as stretching infinitely upwards from \(s = \ln t\) over the segment \(t = 1\) to \(t = 2\), we can confidently establish that there’s no upper boundary for \(s\). This unbounded nature inherently brings improper integration into play.
- The region is bounded below by the curve \(s = \ln t\).
- The region begins at \(t = 1\) and stretches to \(t = 2\).
- For any selected \(t\), \(s\) starts at \(\ln t\) and extends upwards indefinitely.
By visualizing the region as stretching infinitely upwards from \(s = \ln t\) over the segment \(t = 1\) to \(t = 2\), we can confidently establish that there’s no upper boundary for \(s\). This unbounded nature inherently brings improper integration into play.
Limits of Integration
The limits of integration are crucial as they define the interval over which the integration takes place. In this double integral exercise, the limits are based on the region of integration:
Correctly determining and using limits helps ensure that the calculations in solving the integral consider the designated area around which the function is being integrated. Bear in mind that one limit reaching infinity directly leads to an improper integral, presenting challenges such as potential divergence.
- The inner integral: \(s\) spans from \(s = \ln t\) to \(s = \infty\).
- The outer integral: \(t\) reaches from \(t = 1\) to \(t = 2\).
Correctly determining and using limits helps ensure that the calculations in solving the integral consider the designated area around which the function is being integrated. Bear in mind that one limit reaching infinity directly leads to an improper integral, presenting challenges such as potential divergence.
Other exercises in this chapter
Problem 28
Find the area of the region that lies inside the cardioid \(r=1+\cos \theta\) and outside the circle \(r=1.\)
View solution Problem 28
The previous integrals suggest there are preferred orders of integration for spherical coordinates, but other orders give the same value and are occasionally ea
View solution Problem 28
Find the volume of the region bounded above by the plane \(z=y / 2\) and below by the rectangle \(R: 0 \leq x \leq 4,0 \leq y \leq 2\)
View solution Problem 29
Find the area enclosed by one leaf of the rose \(r=12 \cos 3 \theta\).
View solution