Problem 48
Question
Consider \(f(x)=n^{2} x e^{-n x}\). (a) Graph \(f(x)\) for \(n=1,2,3,4,5,6\) on \([0,1]\) in the same graph window. (b) For \(x>0\), find \(\lim _{n \rightarrow \infty} f(x)\). (c) Evaluate \(\int_{0}^{1} f(x) d x\) for \(n=1,2,3,4,5,6\). (d) Guess at \(\lim _{n \rightarrow \infty} \int_{0}^{1} f(x) d x\). Then justify your answer rigorously.
Step-by-Step Solution
Verified Answer
(a) Plot shows peaks shifting leftwards. (b) Limit is 0. (c) Integrals approach 1. (d) Limit is 1 due to diminishing \((n+1)e^{-n}\).
1Step 1: Graphing Multiple Functions
Graph the function \(f(x) = n^2 x e^{-nx}\) for each value \(n = 1, 2, 3, 4, 5, 6\) over the interval \([0, 1]\). Plotting these curves will show how the function changes with different values of \(n\). As \(n\) increases, the peak of the function moves to the left and becomes steeper because the factor \(e^{-nx}\) declines more rapidly.
2Step 2: Finding the Limit as n Approaches Infinity
To find \(\lim_{n \to \infty} f(x)\) for \(x > 0\), note that \(f(x) = n^2 x e^{-nx}\). As \(n\) increases, \(e^{-nx}\) approaches zero very quickly for any \(x > 0\). Thus, the whole function tends toward zero: \(\lim_{n \to \infty} n^2 x e^{-nx} = 0\).
3Step 3: Evaluating the Integral
Compute the integral \(\int_0^1 n^2 x e^{-nx} dx\) for each \(n = 1, 2, 3, 4, 5, 6\). Use integration by parts to solve this. Let \(u = x\) and \(dv = n^2 e^{-nx} dx\). Then \(du = dx\) and \(v = -n e^{-nx}\) (after integrating \(dv\)). The integration by parts formula \(\int u \, dv = uv - \int v \, du\) leads to: \[ \int_0^1 n^2 x e^{-nx} \, dx = \left[ -n x e^{-nx} \right]_0^1 + \int_0^1 n e^{-nx} \, dx = -n e^{-n} - n\left[ \frac{-e^{-nx}}{n} \right]_0^1 \]This simplifies to \(1 - (n+1)e^{-n}\). Evaluate this for each \(n = 1, 2, 3, 4, 5, 6\).
4Step 4: Analyzing the Limit of the Integral
Look at the sequence of evaluated integrals from Step 3 as \(n\) increases. The term \((n+1) e^{-n}\) becomes very small as \(n\) grows, effectively approaching zero. Thus, the integral \(\int_0^1 n^2 x e^{-nx} \, dx\) approaches 1 as \(n \to \infty\). Hence, \(\lim_{n \to \infty} \int_0^1 f(x) \, dx = 1\). The limit relies on the fact that exponential decay in \(e^{-n}\) dominates the linear growth in \(n+1\).
Key Concepts
Exponential DecayIntegration by PartsFunction GraphingLimitsImproper Integrals
Exponential Decay
Exponential decay in mathematical functions often refers to how a quantity decreases rapidly over time or with an increase in a variable, typically denoted by an exponent. In the function given, \(f(x) = n^2 x e^{-nx}\), the term \(e^{-nx}\) decreases rapidly as \(x\) or \(n\) increases.
This characteristic is crucial to understand how the function behaves for different values of \(n\). As \(n\) gets larger, the decay becomes sharper, impacting how the function looks graphically and influences the results of limits and integrals.
Exponential decay is critical when modeling real-world scenarios like radioactive decay or cooling processes, where reducing quantities over a distance or time interval is optimal.
This characteristic is crucial to understand how the function behaves for different values of \(n\). As \(n\) gets larger, the decay becomes sharper, impacting how the function looks graphically and influences the results of limits and integrals.
Exponential decay is critical when modeling real-world scenarios like radioactive decay or cooling processes, where reducing quantities over a distance or time interval is optimal.
Integration by Parts
Integration by parts is a useful technique to solve integrals that are products of two different functions. It is derived from the product rule of differentiation and is particularly valuable when dealing with complex products like \(n^2 x e^{-nx}\).
The formula for integration by parts is given by:\[\int u \, dv = uv - \int v \, du\]Here, we choose \(u = x\) and \(dv = n^2 e^{-nx} dx\).
The formula for integration by parts is given by:\[\int u \, dv = uv - \int v \, du\]Here, we choose \(u = x\) and \(dv = n^2 e^{-nx} dx\).
- Differentiate \(u\) to get \(du = dx\).
- Integrate \(dv\) to find \(v = -n e^{-nx}\).
Function Graphing
Graphing functions is an effective way to visualize how they change with different parameters. For the function \(f(x) = n^2 x e^{-nx}\) for \(n = 1, 2, 3, 4, 5, 6\), plotting helps illustrate the impact of exponential decay visually.
It's observed that
Graphing offers insights into the practical applications of mathematics by showcasing these changes and supporting solutions involving limits and integrals.
It's observed that
- as \(n\) increases,
the peak of the function shifts to the left, - and the slope becomes steeper.
Graphing offers insights into the practical applications of mathematics by showcasing these changes and supporting solutions involving limits and integrals.
Limits
In calculus, a limit helps describe the behavior of a function as a variable approaches a particular value or infinity. For the function \(f(x) = n^2 x e^{-nx}\), finding the limit as \(n\) approaches infinity is fundamental.
For \(x > 0\), observe that \(e^{-nx}\) becomes very small rapidly, thus making \(n^2 x e^{-nx}\) tend towards zero.
This is formally expressed as:\[\lim_{n \to \infty} n^2 x e^{-nx} = 0\]This \(zero\) result demonstrates how exponential decay dominates, ensuring the function value decreases to an infinitesimally small amount as \(n\) becomes very large.
For \(x > 0\), observe that \(e^{-nx}\) becomes very small rapidly, thus making \(n^2 x e^{-nx}\) tend towards zero.
This is formally expressed as:\[\lim_{n \to \infty} n^2 x e^{-nx} = 0\]This \(zero\) result demonstrates how exponential decay dominates, ensuring the function value decreases to an infinitesimally small amount as \(n\) becomes very large.
Improper Integrals
Improper integrals occur when the boundaries of an integral stretch to infinity or the function being integrated becomes infinite within the interval. For this exercise, the integral \(\int_0^1 n^2 x e^{-nx} dx\) concerns an infinite parameter \(n\) eventually approximating an improper integral as \(n \rightarrow \infty\).
Often using integration techniques and limits, as done here, the indefinite growth of \(n\) is tempered by the rapid exponential decay of \(e^{-nx}\).
The particular integral simplifies to:\[1 - (n+1)e^{-n}\] as \(n\) increases.
The exponential part \((n+1)e^{-n}\), approaches zero fast, leading to the integral approaching 1, validating how improper integrals behave and why exponential decay plays such a significant role in their convergence.
Often using integration techniques and limits, as done here, the indefinite growth of \(n\) is tempered by the rapid exponential decay of \(e^{-nx}\).
The particular integral simplifies to:\[1 - (n+1)e^{-n}\] as \(n\) increases.
The exponential part \((n+1)e^{-n}\), approaches zero fast, leading to the integral approaching 1, validating how improper integrals behave and why exponential decay plays such a significant role in their convergence.
Other exercises in this chapter
Problem 46
Let \(c_{1}, c_{2}, \ldots, c_{n}\) be positive constants with \(\sum_{i=1}^{n} c_{i}=1\), and let \(x_{1}, x_{2}, \ldots, x_{n}\) be positive numbers. Take nat
View solution Problem 47
Use the Comparison Test of Problem 46 to show that \(\int_{1}^{\infty} e^{-x^{2}} d x\) converges. Hint: \(e^{-x^{2}} \leq e^{-x}\) on \([1, \infty)\)
View solution Problem 49
Find the absolute maximum and minimum points (if they exist) for \(f(x)=\left(x^{25}+x^{3}+2^{x}\right) e^{-x}\) on \([0, \infty)\).
View solution Problem 53
(Gamma Function) Let \(\Gamma(n)=\int_{0}^{\infty} x^{n-1} e^{-x} d x, n>0 .\) This integral converges by Problems 51 and \(52 .\) Show each of the following (n
View solution