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For each initial value problem, (a) Find the general solution of the differential equation. (b) Impose the initial condition to obtain the solution of the initial value problem. \(2 t y-y^{\prime}=0, \quad y(1)=3\)

Short Answer

Expert verified
Question: Solve the initial value problem \(2ty - y^\prime = 0\) with the initial condition \(y(1) = 3\). Answer: The particular solution of the initial value problem is \(y = \frac{3}{e}e^{t^2}\).

Step by step solution

01

Rewrite the given differential equation in the standard form

From the given differential equation, \(2ty- y^\prime = 0\), we can rewrite it in the standard form \(y^\prime = f(t, y)\). To do this, we will isolate the \(y^\prime\) term: \(y^\prime = 2ty\) Now we have the differential equation in the standard form: \(y^\prime = 2ty\).
02

Solve the differential equation to find the general solution

To solve this first-order linear homogeneous differential equation, we can use the method of separation of variables. Divide both sides by \(y\) and multiply both sides by \(dt\): \(\frac{1}{y}dy = 2tdt\) Now, integrate both sides with respect to the respective variables: \(\int \frac{1}{y} dy = \int 2t dt\) This yields: \(\ln |y| = t^2 + C_1\) To solve for \(y\), we can take the exponential of both sides: \(|y| = e^{t^2 + C_1}\) Since the absolute value of \(y\) is always non-negative, we can use a constant factor \(C = e^{C_1}\) to simplify: \(y = Ce^{t^2}\) Now we have the general solution of the differential equation: \(y = Ce^{t^2}\).
03

Use the initial condition to find the particular solution

We are given the initial condition \(y(1) = 3\). Let us substitute the values of \(t = 1\) and \(y = 3\) into the general solution to find the value of the constant \(C\): \(3 = Ce^{1^2}\) \(\Rightarrow 3 = Ce\) Now we can solve for \(C\): \(C = \frac{3}{e}\) Substitute the value of \(C\) back into the general solution: \(y = \frac{3}{e}e^{t^2}\) Now we have the particular solution of the initial value problem: \(y = \frac{3}{e}e^{t^2}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Differential Equations
Differential equations are mathematical equations that relate some function with its derivatives. They come into play when a rate of change or a relationship that involves some continuous process is part of a scenario, like how a material cools over time or how populations change. Understanding the core idea behind differential equations is crucial because they are not just abstract mathematical constructs. Instead, they model the behavior of variables in dynamic systems, whether in physics, biology, economics, or engineering.

In the given exercise, we encounter a first-order differential equation. This means that it involves the first derivative of the unknown function, represented by the notation \( y' \). The differential equation \( 2ty - y' = 0 \) captures how the rate of change of the function \( y \) with respect to the variable \( t \) is directly related to the product of \( t \) and \( y \) itself.
General Solution
The general solution to a differential equation represents a family of solutions containing arbitrary constants. In the context of our initial value problem, finding the general solution involves determining the form of the function y that can satisfy the given differential equation for all values of the independent variable t.

Obtaining the General Solution

Given the equation \( y' = 2ty \), the general solution is obtained by separating and integrating both sides. The result, \( y = Ce^{t^2} \), includes an undetermined constant \( C \), signifying an infinite set of possible solutions. This stage is critical as it sets the stage for further refinement of the solution by incorporating initial conditions.
Particular Solution
While the general solution gives us a broad set of solutions, a particular solution is one specific member of this family that satisfies the initial value conditions of the problem. To find it, we use the given initial condition \( y(1) = 3 \).

Applying the Initial Condition

By substituting \( t = 1 \) and \( y = 3 \) into our general solution, we can solve for the constant \( C \). This process tailors the general solution to a unique scenario outlined by the initial conditions, resulting in the particular solution \( y = \frac{3}{e}e^{t^2} \), which uniquely satisfies both the differential equation and the initial condition.
Separation of Variables
Separation of variables is a commonly used method for solving first-order differential equations. It involves rearranging the equation to isolate the derivatives of each variable on opposite sides of the equation.

Implementing Separation of Variables

In our exercise, we have \( y' = 2ty \). By dividing both sides by \( y \) and multiplying both sides by the differential \( dt \), the variables \( y \) and \( t \) become separated. We then proceed to integrate both sides, leading us to the general solution. This technique fundamentally breaks down a complex relationship into simple, integrable parts, allowing us to find the general solution with comparative ease.

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Most popular questions from this chapter

An object undergoes one-dimensional motion along the \(x\)-axis subject to the given decelerating forces. At time \(t=0\), the object's position is \(x=0\) and its velocity is \(v=v_{0}\). In each case, the decelerating force is a function of the object's position \(x(t)\) or its velocity \(v(t)\) or both. Transform the problem into one having distance \(x\) as the independent variable. Determine the position \(x_{f}\) at which the object comes to rest. (If the object does not come to rest, \(x_{f}=\infty\).) $$ m \frac{d v}{d t}=-\frac{k v}{1+x} $$

If \(y(t)=3 e^{t^{2}}\) is known to be the solution of the initial value problem $$ y^{\prime}+p(t) y=0, \quad y(0)=y_{0}, $$ what must the function \(p(t)\) and the constant \(y_{0}\) be?

On August 24,1894 , Pop Shriver of the Chicago White Stockings caught a baseball dropped (by Clark Griffith) from the top of the Washington Monument. The Washington Monument is \(555 \mathrm{ft}\) tall and a baseball weighs \(5 \frac{1}{8} \mathrm{oz}\). (a) If we ignore air resistance and assume the baseball was acted upon only by gravity, how fast would the baseball have been traveling when it was \(7 \mathrm{ft}\) above the ground? (b) Suppose we now include air resistance in our model, assuming that the drag force is proportional to velocity with a drag coefficient \(k=0.0018 \mathrm{lb}-\mathrm{sec} / \mathrm{ft}\). How fast is the baseball traveling in this case when it is \(7 \mathrm{ft}\) above the ground?

Consider a population modeled by the initial value problem $$ \frac{d P}{d t}=(1-P) P+M, \quad P(0)=P_{0} $$ where the migration rate \(M\) is constant. [The model (8) is derived from equation (6) by setting the constants \(r\) and \(P_{*}\) to unity. We did this so that we can focus on the effect \(M\) has on the solutions.] For the given values of \(M\) and \(P(0)\), (a) Determine all the equilibrium populations (the nonnegative equilibrium solutions) of differential equation (8). As in Example 1, sketch a diagram showing those regions in the first quadrant of the \(t P\)-plane where the population is increasing \(\left[P^{\prime}(t)>0\right]\) and those regions where the population is decreasing \(\left[P^{\prime}(t)<0\right]\). (b) Describe the qualitative behavior of the solution as time increases. Use the information obtained in (a) as well as the insights provided by the figures in Exercises 11-13 (these figures provide specific but representative examples of the possibilities). $$ M=-\frac{1}{4}, \quad P(0)=\frac{1}{4} $$

(a) Obtain an implicit solution and, if possible, an explicit solution of the initial value problem. (b) If you can find an explicit solution of the problem, determine the \(t\)-interval of existence. $$ e^{t} y^{\prime}+(\cos y)^{2}=0, \quad y(0)=\pi / 4 $$

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