Problem 18
Question
From \(\frac{1}{N} d N=\left(t e^{t+2}-1\right) d t\) we obtain \(\ln |N|=t e^{t+2}-e^{t+2}-t+c\) or \(N=c_{1} e^{t e^{t+2}-e^{t+2}-t}\).
Step-by-Step Solution
Verified Answer
\( N = c_1 e^{t e^{t+2} - e^{t+2} - t} \).
1Step 1: Introduce the Given Differential Equation
We start with the given equation \( \frac{1}{N} \, dN = (t e^{t+2} - 1) \, dt \). This is a separable differential equation, allowing us to separate the variables \( N \) and \( t \).
2Step 2: Separate Variables and Integrate
Separate the variables to get \( \int \frac{1}{N} \, dN = \int (t e^{t+2} - 1) \, dt \). Integrate both sides: \( \ln |N| = \int t e^{t+2} \, dt - \int 1 \, dt \).
3Step 3: Solve the First Integral
To solve \( \int t e^{t+2} \, dt \), use integration by parts. Let \( u = t \) and \( dv = e^{t+2} \, dt \). Then \( du = dt \) and \( v = e^{t+2} \). The integration by parts formula is \( \int u \, dv = uv - \int v \, du \).
4Step 4: Apply Integration by Parts
Applying the formula: \( \int t e^{t+2} \, dt = t e^{t+2} - \int e^{t+2} \, dt \). The second integral is straightforward: \( \int e^{t+2} \, dt = e^{t+2} + C \), so \( \int t e^{t+2} \, dt = t e^{t+2} - e^{t+2} \).
5Step 5: Solve the Second Integral
The second integral \( \int 1 \, dt = t \). Add the constant \( C \) for the indefinite integrals: \( \ln |N| = t e^{t+2} - e^{t+2} - t + C \).
6Step 6: Solve for N
Exponentiate both sides to solve for \( N \): \( |N| = e^{t e^{t+2} - e^{t+2} - t + C} \). Simplify to \( N = c_1 e^{t e^{t+2} - e^{t+2} - t} \), where \( c_1 = e^C \) is an arbitrary constant.
Key Concepts
Integration by PartsDifferential Equation SolutionsIndefinite Integrals
Integration by Parts
Integration by parts is a powerful technique used to solve integrals involving the product of two functions. It is especially handy when one of the functions easily integrates while the other simplifies when differentiated.
To apply integration by parts, we use the formula:
For example, in the integral \( \int t e^{t+2} \, dt \), we select \( u = t \) and \( dv = e^{t+2} \, dt \). This choice simplifies the calculations as \( du = dt \) and \( v = e^{t+2} \), forming a straightforward integration.
The final calculation results in \( t e^{t+2} - e^{t+2} \), which is much simpler to handle in further computations.
To apply integration by parts, we use the formula:
- \( \int u \, dv = uv - \int v \, du \)
For example, in the integral \( \int t e^{t+2} \, dt \), we select \( u = t \) and \( dv = e^{t+2} \, dt \). This choice simplifies the calculations as \( du = dt \) and \( v = e^{t+2} \), forming a straightforward integration.
The final calculation results in \( t e^{t+2} - e^{t+2} \), which is much simpler to handle in further computations.
Differential Equation Solutions
Differential equations involve derivatives and are used to describe various physical phenomena. Solving them often means finding a function that satisfies the given relationship between variables.
In the exercise, we are working with a separable differential equation, which allows us to rearrange terms so each variable occupies its own side of the equation. This makes it easier to integrate each part separately.
Starting with \( \frac{1}{N} \, dN = (t e^{t+2} - 1) \, dt \), we can separate and then integrate both sides:
The solution to the differential equation, \( N = c_1 e^{t e^{t+2}-e^{t+2} - t} \), provides the general form of the function \( N(t) \).
In the exercise, we are working with a separable differential equation, which allows us to rearrange terms so each variable occupies its own side of the equation. This makes it easier to integrate each part separately.
Starting with \( \frac{1}{N} \, dN = (t e^{t+2} - 1) \, dt \), we can separate and then integrate both sides:
- \( \int \frac{1}{N} \, dN = \ln |N| \)
- \( \int (t e^{t+2} - 1) \, dt \) involves using integration by parts for \( t e^{t+2} \) and a simple integral for \( -1 \).
The solution to the differential equation, \( N = c_1 e^{t e^{t+2}-e^{t+2} - t} \), provides the general form of the function \( N(t) \).
Indefinite Integrals
Indefinite integrals represent families of functions and include a constant of integration, symbolized as \( C \), because their derivative yields the original function being integrated.
In our exercise, we encounter indefinite integrals such as:
Integrating results in expressions that contain \( C \), reminding us that without specific boundary conditions or additional information, our solutions remain generalized.
Indefinite integrals thus offer flexibility but require further data to specify unique solutions.
In our exercise, we encounter indefinite integrals such as:
- \( \int \frac{1}{N} \, dN = \ln |N| + C \)
- \( \int (t e^{t+2} - 1) \, dt \), which breaks into two separate integrals using integration by parts and basic rules.
Integrating results in expressions that contain \( C \), reminding us that without specific boundary conditions or additional information, our solutions remain generalized.
Indefinite integrals thus offer flexibility but require further data to specify unique solutions.
Other exercises in this chapter
Problem 18
(a) Writing the equation in the form \((x-\sqrt{x^{2}+y^{2}}) d x+y d y=0\) we identify \(M=x-\sqrt{x^{2}+y^{2}}\) and \(N=y\) since \(M\) and \(N\) are both ho
View solution Problem 18
(a) The initial temperature of the bath is \(T_{m}(0)=60^{\circ},\) so in the short term the temperature of the chemical, which starts at \(80^{\circ},\) should
View solution Problem 18
From \(y^{\prime}-\left(1+\frac{1}{x}\right) y=y^{2}\) and \(w=y^{-1}\) we obtain \(\frac{d w}{d x}+\left(1+\frac{1}{x}\right) w=-1\). An integrating factor is
View solution Problem 18
For \(y^{\prime}+(\cot x) y=\sec ^{2} x \csc x\) an integrating factor is \(e^{\int \cot x d x}=e^{\ln |\sin x|}=\sin x\) so that \(\frac{d}{d x}[(\sin x) y]=\s
View solution