Problem 69
Question
The pressure \(P\) and temperature \(T\) in the outer envelope of a white dwarf (star) are related by the differential equation $$ \frac{d P}{d T}=C \frac{T^{7.5}}{P}, P(0)=0 $$ where \(C\) is a constant. Find \(P\) as a function of \(T\).
Step-by-Step Solution
Verified Answer
The pressure as a function of temperature is \( P(T) = \sqrt{\frac{2C}{8.5}} T^{4.25} \).
1Step 1: Separate the Variables
Start by rearranging the given differential equation \( \frac{d P}{d T}=C \frac{T^{7.5}}{P} \) to isolate variables involving \( P \) on one side and those involving \( T \) on the other side. Multiply both sides by \( P \) and \( dT \) to obtain \( P \, dP = C \, T^{7.5} \, dT \).
2Step 2: Integrate Both Sides
Integrate both sides of the equation. The integration on the left-hand side with respect to \( P \) is \( \int P \, dP = \frac{P^2}{2} \) and on the right-hand side with respect to \( T \), it is \( \int C \, T^{7.5} \, dT = C \frac{T^{8.5}}{8.5} + D \), where \(D\) is the constant of integration.
3Step 3: Solve for Constant of Integration
Since the initial condition given is \( P(0) = 0 \), substitute this into the integrated equation: \( \frac{0^2}{2} = C \frac{0^{8.5}}{8.5} + D \). This simplifies to \( D = 0 \).
4Step 4: Solve for P
Now, write the equation obtained from the integration with known constant \(D\): \( \frac{P^2}{2} = C \frac{T^{8.5}}{8.5} \). Solve for \(P\): \( P = \sqrt{\frac{2C}{8.5} T^{8.5}} = \sqrt{\frac{2CT^{8.5}}{8.5}} \). This gives the relationship \( P(T) = \sqrt{\frac{2C}{8.5}} T^{4.25} \).
Key Concepts
Separation of VariablesIntegrationInitial Value Problem
Separation of Variables
Separation of variables is a fundamental method used to solve certain kinds of differential equations. When an equation involves two variables, say \( P \) and \( T \), you can often separate the variables by manipulating the equation into two distinct parts, each containing only one of the variables.
This technique is particularly useful when dealing with equations that can be rearranged so that all terms involving one variable are on one side of the equation and all terms involving the other variable are on the opposite side.
In our exercise, we separated the variables by multiplying both sides of the equation by \( P \) and \( dT \), which rearranged the equation into:
This technique is particularly useful when dealing with equations that can be rearranged so that all terms involving one variable are on one side of the equation and all terms involving the other variable are on the opposite side.
In our exercise, we separated the variables by multiplying both sides of the equation by \( P \) and \( dT \), which rearranged the equation into:
- \( P \, dP = C \, T^{7.5} \, dT \)
Integration
Integration is the process of finding the integral of a function, which is essentially the opposite of differentiating. It is a vital step in solving differential equations after variables have been separated. There are two main components when integrating: the integral function and the constant of integration.
In the context of the exercise, integrating both sides of the equation was the next logical step after separating the variables. Each side of the equation correlates to a different variable, and we integrate separately with respect to each variable.
For example, the integration process on the left side for \( P \) includes the integral:
In the context of the exercise, integrating both sides of the equation was the next logical step after separating the variables. Each side of the equation correlates to a different variable, and we integrate separately with respect to each variable.
For example, the integration process on the left side for \( P \) includes the integral:
- \( \int P \, dP = \frac{P^2}{2} \)
- \( \int C \, T^{7.5} \, dT = C \frac{T^{8.5}}{8.5} + D \)
Initial Value Problem
An initial value problem is a type of differential equation that provides additional conditions, known as initial conditions, to determine a unique solution. These conditions specify the value of the unknown function at a specific point, which helps in finding the exact form of the solution.
In the given exercise, the initial condition provided is \( P(0) = 0 \). This means that when the temperature \( T \) is zero, the pressure \( P \) should also be zero.
The initial condition is crucial for determining the constant of integration. By substituting \( T = 0 \) into our integrated function, we find:
In the given exercise, the initial condition provided is \( P(0) = 0 \). This means that when the temperature \( T \) is zero, the pressure \( P \) should also be zero.
The initial condition is crucial for determining the constant of integration. By substituting \( T = 0 \) into our integrated function, we find:
- \( \frac{0^2}{2} = C \frac{0^{8.5}}{8.5} + D \)
Other exercises in this chapter
Problem 69
Find the center of mass of the given region \(\mathcal{R}\) \(\mathcal{R}\) is bounded above by \(y=\ln \left(1+x+x^{2}\right)\) and below by \(y=x^{2}-3\)
View solution Problem 69
In each of Exercises 69-76, calculate the volume of the solid obtained when the region \(\mathcal{R}\) is rotated about the given line \(\ell\) \(\mathcal{R}\)
View solution Problem 70
In each of Exercises \(65-74\) calculate the expectation of a random variable whose probability density function is given. $$ \frac{4 \arctan (x)}{\pi-2 \ln (2)
View solution Problem 70
In each of Exercises 69-76, calculate the volume of the solid obtained when the region \(\mathcal{R}\) is rotated about the given line \(\ell\) \(\mathcal{R}\)
View solution