Problem 60
Question
The acceleration of a particle moving back and forth on a line is \(a=d^{2} s / d t^{2}=\pi^{2} \cos \pi t \mathrm{m} / \mathrm{sec}^{2}\) for all \(t .\) If \(s=0\) and \(v=\) 8 \(\mathrm{m} / \mathrm{sec}\) when \(t=0,\) find \(s\) when \(t=1 \mathrm{sec} .\)
Step-by-Step Solution
Verified Answer
The position \(s\) when \(t = 1\) second is 10 meters.
1Step 1: Understand the Relationship Between Acceleration, Velocity, and Position
The problem provides the function for acceleration of the particle, given by \(a = \frac{d^2s}{dt^2} = \pi^2 \cos(\pi t)\). We need to find the position \(s\) at time \(t = 1\). To do this, we first need to integrate the acceleration to find the velocity function, and then integrate the velocity to find the position function.
2Step 2: Integrate Acceleration to Find Velocity
Integrate the acceleration function to determine the velocity: \[ v = \int a \, dt = \int \pi^2 \cos(\pi t) \, dt. \]The integration gives: \[ v(t) = \pi \sin (\pi t) + C_1, \]where \(C_1\) is the integration constant. We will determine this from the initial condition \(v(0) = 8\).
3Step 3: Apply Initial Condition to Find Constant of Integration for Velocity
Using the initial condition \(v(0) = 8\ mu s/\text{sec}\), substitute \(t = 0\) into the velocity equation: \[ v(0) = \pi \sin(0) + C_1 = 8. \]Since \(\sin(0) = 0\), it simplifies to \(C_1 = 8\). Therefore, the velocity function is:\[ v(t) = \pi \sin(\pi t) + 8. \]
4Step 4: Integrate Velocity to Find Position
Integrate the velocity function to determine the position:\[ s = \int v(t) \, dt = \int (\pi \sin(\pi t) + 8) \, dt. \]This simplifies to:\[ s(t) = -\cos(\pi t) + 8t + C_2, \]where \(C_2\) is another constant of integration that we will find using the initial condition \(s(0) = 0\).
5Step 5: Apply Initial Condition to Find Constant of Integration for Position
Using the initial condition \(s(0) = 0\), substitute \(t = 0\) into the position equation:\[ s(0) = -\cos(0) + 8(0) + C_2 = 0. \]Since \(-\cos(0) = -1\), it simplifies to \(-1 + C_2 = 0\), leading to \(C_2 = 1\). Thus, the position function is:\[ s(t) = -\cos(\pi t) + 8t + 1. \]
6Step 6: Substitute t = 1 to Find s(1)
Substitute \(t = 1\) into the position function:\[ s(1) = -\cos(\pi \times 1) + 8(1) + 1. \]Since \(\cos(\pi) = -1\), this becomes:\[ s(1) = -(-1) + 8 + 1 = 1 + 8 + 1 = 10. \]
Key Concepts
Acceleration IntegrationInitial Conditions in CalculusPosition Function Calculation
Acceleration Integration
One central concept in this problem is acceleration integration. In physics and calculus, acceleration is the rate of change of velocity over time. If we have an expression for acceleration, we can reverse this process, through integration, to find the velocity.
In our exercise, the acceleration is firstly expressed as a function of time:
When we integrate the given acceleration equation:
In our exercise, the acceleration is firstly expressed as a function of time:
- \( a(t) = \pi^2 \cos(\pi t) \)
When we integrate the given acceleration equation:
- \( v(t) = \int \pi^2 \cos(\pi t) \, dt \)
- \( v(t) = \pi \sin (\pi t) + C_1 \)
Initial Conditions in Calculus
Initial conditions in calculus are vital for determining the exact form of a solution after integration. Each integration introduces a constant, because indefinitely many functions can have the same derivative.
In our case, the acceleration equation's integration to get velocity yields a constant \( C_1 \). To solve for this, we use the initial condition, specifying that initially (after our first calculation point) the velocity, \( v(0) \), equals 8 m/s.
Similarly, integrating the velocity gives us the position function with another constant, \( C_2 \). Using \( s(0) = 0 \) allows us to solve for \( C_2 \):
Such conditions ensure our final function accurately reflects the particle's motion in reality.
In our case, the acceleration equation's integration to get velocity yields a constant \( C_1 \). To solve for this, we use the initial condition, specifying that initially (after our first calculation point) the velocity, \( v(0) \), equals 8 m/s.
- Setting \( v(0) = \pi \sin(0) + C_1 = 8 \)
Similarly, integrating the velocity gives us the position function with another constant, \( C_2 \). Using \( s(0) = 0 \) allows us to solve for \( C_2 \):
- \( s(0) = -\cos(0) + 8(0) + C_2 = 0 \)
Such conditions ensure our final function accurately reflects the particle's motion in reality.
Position Function Calculation
In calculus, a position function specifies the location of an object at any given time. It's derived by integrating the velocity function, which itself comes from the integrated acceleration.
Our exercise required finding the position of a particle. We had already identified velocity as:
Finally, to find \( s(1) \), representing position at 1 second, we evaluate the function at \( t = 1 \):
Our exercise required finding the position of a particle. We had already identified velocity as:
- \( v(t) = \pi \sin(\pi t) + 8 \)
- \( s(t) = \int (\pi \sin(\pi t) + 8) \, dt \)
- \( s(t) = -\cos(\pi t) + 8t + 1 \)
Finally, to find \( s(1) \), representing position at 1 second, we evaluate the function at \( t = 1 \):
- \( s(1) = -\cos(\pi \cdot 1) + 8 \cdot 1 + 1 \)
- This equals \( 10 \), revealing the particle's position as 10 meters at \( t = 1 \) second.
Other exercises in this chapter
Problem 59
In Exercises \(55-62,\) graph the function and find its average value over the given interval. $$ f(t)=(t-1)^{2} \quad \text { on } \quad[0,3] $$
View solution Problem 60
Find the areas of the regions enclosed by the curves in Exercises \(59-62\). $$ x^{3}-y=0 \quad \text { and } \quad 3 x^{2}-y=4 $$
View solution Problem 60
In Exercises \(55-62,\) graph the function and find its average value over the given interval. $$ f(t)=t^{2}-t \quad \text { on } \quad[-2,1] $$
View solution Problem 61
It looks as if we can integrate 2 sin \(x \cos x\) with respect to \(x\) in three different ways: $$ \begin{aligned} \text { a. } \int 2 \sin x \cos x d x &=\in
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