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If \(p(t)\) is any function continuous on an interval of the form \(a

Short Answer

Expert verified
Answer: The unique solution of the given initial value problem is \(y(t) = 0\).

Step by step solution

01

Identify the given problem

We are tasked with identifying the unique solution of the initial value problem: $$ y'(t) + p(t) y = 0, \quad y(t_0) = 0 $$ where \(p(t)\) is continuous on an interval \((a, b)\) and \(t_0 \in (a, b)\).
02

Analyzing the given problem

The given initial value problem can be represented as a first-order linear differential equation. In order to solve the problem, we will try to identify one solution by inspection and then apply Theorem 2.1 to prove that it must be the unique solution.
03

Identifying one solution by inspection

Notice that if we plug in \(y(t) = 0\), the given differential equation becomes: $$ 0' + p(t) \cdot 0 = 0 $$ Since \(0' = 0\), the equation simplifies to: $$ 0 = 0 $$ This means that \(y(t) = 0\) is a solution of the given differential equation, and it satisfies the initial condition \(y(t_0) = 0\).
04

Apply Theorem 2.1

Theorem 2.1 states that if an initial value problem has a solution, it must be unique. Since we have found a solution \(y(t) = 0\) by inspection, we can conclude that this solution is unique. There is no other solution that will satisfy both the given differential equation and the initial condition on the interval \((a, b)\).
05

Write out the unique solution

The unique solution of the given initial value problem is: $$ y(t) = 0 $$

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Key Concepts

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

Initial Value Problem
An initial value problem is a type of differential equation that has a specific initial condition at a particular point. In our problem, we have the differential equation given by the expression \( y'(t) + p(t) y = 0 \), where the function \( y(t) \) needs to satisfy the initial condition \( y(t_0) = 0 \). The initial value \( t_0 \) provides a starting point within the interval \( (a, b) \).
Solving an initial value problem requires finding a function \( y(t) \) that not only satisfies the differential equation but also the condition at \( t_0 \). This makes initial value problems significant as they provide clear criteria that the solution must meet at a specific point on the interval.
Continuous Functions
In this context, the function \( p(t) \) is described as continuous over the interval \( (a, b) \). A continuous function is one that doesn’t have any breaks, jumps, or holes in its domain. This means for every point in the interval, there is a corresponding function value, and small changes in \( t \) results in small changes in \( p(t) \).
Such continuity ensures stability in the behavior of the differential equation, which helps in the analysis and finding the solution. For instance, because \( p(t) \) is continuous, it is easier to deduce that if \( y(t) = 0 \) is a solution on the whole interval, then it is consistent throughout without any disturbances or anomalies. This consistency plays a critical role in ensuring the equation's predictability and the uniqueness of its solution.
Unique Solution
The uniqueness of a solution in a differential equation context ensures that within the constraints given by initial conditions, there is only one function that fulfills both the differential equation and the initial condition at \( t_0 \).
For our problem, using Theorem 2.1, which deals with the uniqueness of solutions for linear differential equations, we can ascertain that the solution \( y(t) = 0 \) is not just a solution but the only solution. The theorem essentially guarantees that no other function can satisfy both the equation \( y'(t) + p(t) y = 0 \) and the initial condition \( y(t_0) = 0 \) within the interval \( (a, b) \).
  • This is crucial because it simplifies the solution process.
  • Students can confidently use \( y(t) = 0 \) knowing it's the unique answer.
Differential Equations
Differential equations form a pivotal part of mathematics and applied sciences as they describe the change in systems. A first-order linear differential equation, like the one given \( y'(t) + p(t)y = 0 \), involves the derivative of a function and it tells us about the rate of change of some quantity.
The power of differential equations lies in their ability to model real-world phenomena, such as physics, engineering, and economics. In simple terms, they help describe how a particular quantity evolves over time given an initial state and a rule (the differential equation).
In our context, solving the differential equation \( y'(t) + p(t)y = 0 \) involves finding a function \( y(t) \) that remains stable over the interval and matches the given initial condition. This equation is particularly simplified to \( y(t) = 0 \) because this solution satisfies both the derivative condition and the initial value all through the defined interval.

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Most popular questions from this chapter

A tank initially holds 500 gal of a brine solution having a concentration of \(0.1 \mathrm{lb}\) of salt per gallon. At some instant, fresh water begins to enter the tank at a rate of 10 \(\mathrm{gal} / \mathrm{min}\) and the well- stirred mixture leaves at the same rate. How long will it take before the concentration of salt is reduced to \(0.01 \mathrm{lb} / \mathrm{gal}\) ?

(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. $$ 3 y^{2} \frac{d y}{d t}+2 t=1, \quad y(-1)=-1 $$

An object of mass \(m\) is dropped from a high platform at time \(t=0\). Assume the drag force is proportional to the square of the velocity, with drag coefficient \(\kappa\). As in Example 1, derive an expression for the velocity \(v(t)\).

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, \(x_{f}=\infty\).) $$ m \frac{d v}{d t}=-\frac{k v}{1+x} $$

Oscillating Flow Rate A tank initially contains \(10 \mathrm{lb}\) of solvent in \(200 \mathrm{gal}\) of water. At time \(t=0\), a pulsating or oscillating flow begins. To model this flow, we assume that the input and output flow rates are both equal to \(3+\sin t \mathrm{gal} / \mathrm{min}\). Thus, the flow rate oscillates between a maximum of \(4 \mathrm{gal} / \mathrm{min}\) and a \(\mathrm{minimum}\) of \(2 \mathrm{gal} / \mathrm{min}\); it repeats its pattern every \(2 \pi \approx 6.28 \mathrm{~min}\). Assume that the inflow concentration remains constant at \(0.5 \mathrm{lb}\) of solvent per gallon. (a) Does the amount of solution in the tank, \(V\), remain constant or not? Explain. (b) Let \(Q(t)\) denote the amount of solvent (in pounds) in the tank at time \(t\) (in minutes). Explain, on the basis of physical reasoning, whether you expect the amount of solvent in the tank to approach an equilibrium value or not. In other words, do you expect \(\lim _{t \rightarrow \infty} Q(t)\) to exist and, if so, what is this limit? (c) Formulate the initial value problem to be solved. (d) Solve the initial value problem. Determine \(\lim _{t \rightarrow \infty} Q(t)\) if it exists.

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