Chapter 12: Problem 46
Solve the vector initial-value problem for \(\mathbf{y}(t)\) by integrating and using the initial conditions to find the constants of integration. $$ \mathbf{y}^{\prime}(t)=\cos t \mathbf{i}+\sin t \mathbf{j}, \mathbf{y}(0)=\mathbf{i}-\mathbf{j} $$
Short Answer
Expert verified
\( \mathbf{y}(t) = (\sin t + 1) \, \mathbf{i} - \cos t \, \mathbf{j} \)
Step by step solution
01
Understand the Problem
We need to find the vector function \( \mathbf{y}(t) \) given its derivative \( \mathbf{y}'(t) \) and initial condition \( \mathbf{y}(0) \). The derivative is given as \( \mathbf{y}'(t) = \cos t \, \mathbf{i} + \sin t \, \mathbf{j} \).
02
Integrate the Derivative
Integrate the components of \( \mathbf{y}'(t) \) separately. Integrating \( \cos t \) with respect to \( t \) gives \( \sin t \), and integrating \( \sin t \) with respect to \( t \) gives \(-\cos t \). Thus, the general solution for \( \mathbf{y}(t) \) is \( \mathbf{y}(t) = \sin t \, \mathbf{i} - \cos t \, \mathbf{j} + \mathbf{C} \), where \( \mathbf{C} \) is a constant vector of integration.
03
Apply the Initial Condition
Use the initial condition \( \mathbf{y}(0) = \mathbf{i} - \mathbf{j} \) to find \( \mathbf{C} \). Substitute \( t = 0 \) into the solution: \( \sin(0) \, \mathbf{i} - \cos(0) \, \mathbf{j} + \mathbf{C} = \mathbf{i} - \mathbf{j} \). This simplifies to \( -\mathbf{j} + \mathbf{C} = \mathbf{i} - \mathbf{j} \). Thus, \( \mathbf{C} = \mathbf{i} \).
04
Substitute the Constant into the General Solution
Now that we have \( \mathbf{C} = \mathbf{i} \), substitute it back into the general solution from Step 2: \( \mathbf{y}(t) = \sin t \, \mathbf{i} - \cos t \, \mathbf{j} + \mathbf{i} \). Thus, \( \mathbf{y}(t) = (\sin t + 1) \, \mathbf{i} - \cos t \, \mathbf{j} \).
05
Final Solution
The final solution for the vector initial-value problem is \( \mathbf{y}(t) = (\sin t + 1) \, \mathbf{i} - \cos t \, \mathbf{j} \).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Initial Value Problem
In mathematics, an Initial Value Problem (IVP) is a type of differential equation along with a given condition called the initial condition. This problem involves finding a function that satisfies a given derivative, along with certain values of the function at a specific point.
In the context of vector calculus, the goal is often to find a vector function whose derivative matches a given vector derivative, typically involving initial values for specific components.
The initial condition serves as a starting point that helps pinpoint the exact solution amongst a family of potential solutions. One important aspect to remember is:
In the context of vector calculus, the goal is often to find a vector function whose derivative matches a given vector derivative, typically involving initial values for specific components.
The initial condition serves as a starting point that helps pinpoint the exact solution amongst a family of potential solutions. One important aspect to remember is:
- The initial condition helps eliminate the constant of integration.
- It ensures the solution is unique to the problem.
Vector Integration
Vector integration in calculus involves integrating vector-valued functions. Each component of the vector is integrated individually with respect to the variable, often time, \(t\).
Just like scalar integration, this process results in a constant of integration - represented as a vector. Consider the vector derivative \(\mathbf{y}'(t) = \cos t \, \mathbf{i} + \sin t \, \mathbf{j}\) from the original problem:
Just like scalar integration, this process results in a constant of integration - represented as a vector. Consider the vector derivative \(\mathbf{y}'(t) = \cos t \, \mathbf{i} + \sin t \, \mathbf{j}\) from the original problem:
- To solve, we integrate \(\cos t\) to get \(\sin t\), and \(\sin t\) to obtain \(-\cos t\).
- This gives us the general solution \(\mathbf{y}(t) = \sin t \, \mathbf{i} - \cos t \, \mathbf{j} + \mathbf{C} \), where \(\mathbf{C}\) is a constant vector.
Vector Functions
Vector functions are functions that return a vector as their output. In vector calculus, these functions often describe physical concepts like velocity or force in terms of vectors, which have both magnitude and direction.
The notation \(\mathbf{y}(t)\) indicates that \(\mathbf{y}\) is a function of \(t\) and produces a vector result.
Let's examine the solution \(\mathbf{y}(t) = (\sin t + 1) \, \mathbf{i} - \cos t \, \mathbf{j}\):
The notation \(\mathbf{y}(t)\) indicates that \(\mathbf{y}\) is a function of \(t\) and produces a vector result.
Let's examine the solution \(\mathbf{y}(t) = (\sin t + 1) \, \mathbf{i} - \cos t \, \mathbf{j}\):
- This solution represents the vector function where each component \(\sin t + 1\) and \(-\cos t\) describes the paths traced in a multidimensional space.
- \(\mathbf{i}\) and \(\mathbf{j}\) are unit vectors, illustrating directions in a Cartesian coordinate system.