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The acceleration of a particle is defined by the relation \(a=3 e^{-0.2 t},\) where \(a\) and \(t\) are expressed in \(\mathrm{ft} / \mathrm{s}^{2}\) and seconds, respectively. Knowing that \(x=0\) and \(v=0\) at \(t=0,\) determine the velocity and position of the particle when \(t=0.5 \mathrm{s}\).

Short Answer

Expert verified
Velocity at \( t = 0.5 \) s is approximately 1.428 ft/s, and position is approximately 0.36 ft.

Step by step solution

01

Understand the Problem

We need to determine the velocity and position of a particle at time \( t = 0.5 \) s, given the acceleration function \( a(t) = 3e^{-0.2t} \), as well as the initial conditions \( v(0) = 0 \) ft/s and \( x(0) = 0 \) ft.
02

Find Velocity Function

The velocity \( v(t) \) can be found by integrating the acceleration function \( a(t) \). Integrate \( a(t) = 3e^{-0.2t} \) with respect to \( t \): \[ v(t) = \int 3e^{-0.2t} \, dt = \left(-\frac{3}{0.2}\right)e^{-0.2t} + C \].\( C \) is the integration constant. Simplifying gives: \[ v(t) = -15e^{-0.2t} + C\].
03

Apply Initial Condition for Velocity

Use the initial condition \( v(0) = 0 \) to find \( C \). Substitute \( t = 0 \) and \( v(0) = 0 \) into the velocity equation: \[ 0 = -15e^{0} + C \rightarrow 0 = -15 + C \rightarrow C = 15 \]. Thus, the velocity function becomes \( v(t) = -15e^{-0.2t} + 15 \).
04

Calculate Velocity at \( t = 0.5 \) s

Substitute \( t = 0.5 \) into the velocity function: \[ v(0.5) = -15e^{-0.2(0.5)} + 15 \]. Calculate the value: \[ v(0.5) = -15e^{-0.1} + 15 \]. Use the approximation \( e^{-0.1} \approx 0.9048 \): \[ v(0.5) \approx -15(0.9048) + 15 = -13.572 + 15 \approx 1.428 \, \text{ft/s}\].
05

Find Position Function

The position \( x(t) \) can be found by integrating the velocity function \( v(t) = -15e^{-0.2t} + 15 \). Integrate with respect to \( t \): \[ x(t) = \int (-15e^{-0.2t} + 15) \, dt = \left(\frac{15}{0.2}\right)e^{-0.2t} + 15t + C_1 \]. Simplify: \[ x(t) = 75e^{-0.2t} + 15t + C_1 \].
06

Apply Initial Condition for Position

Use the initial condition \( x(0) = 0 \) to find \( C_1 \). Substitute \( t = 0 \) and \( x(0) = 0 \) into the position equation: \[ 0 = 75e^{0} + 0 + C_1 \rightarrow 0 = 75 + C_1 \rightarrow C_1 = -75 \]. Thus, the position function becomes \( x(t) = 75e^{-0.2t} + 15t - 75 \).
07

Calculate Position at \( t = 0.5 \) s

Substitute \( t = 0.5 \) into the position function: \[ x(0.5) = 75e^{-0.1} + 15(0.5) - 75\]. Calculate the value using \( e^{-0.1} \approx 0.9048 \): \[ x(0.5) = 75(0.9048) + 7.5 - 75\]. \[ x(0.5) = 67.86 - 75 + 7.5 \approx 0.36 \, \text{ft} \].

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Key Concepts

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

Acceleration Function
An acceleration function describes how a particle's velocity changes over time. In our problem, the acceleration function is given by \( a(t) = 3e^{-0.2t} \). This tells us that the acceleration of the particle changes exponentially with time, specifically decreasing as \( t \) increases. The negative exponent indicates a decaying factor, meaning the rate of acceleration reduces as time passes. Understanding this function helps us predict how the particle's motion will evolve, setting the foundation for finding other related quantities like velocity and position.
Key points about acceleration functions:
  • They are typically given as functions of time \( t \).
  • They can tell us how quickly or slowly the velocity of the particle is changing.
  • Knowing the function helps us derive velocity, through integration, since acceleration is the derivative of velocity.
Integration
Integration is a crucial mathematical tool used to find quantities like velocity and position when given an acceleration function. It essentially reverses differentiation.
When dealing with acceleration \( a(t) \), integrating it yields the velocity function \( v(t) \). Similarly, integrating the velocity function gives us the position function \( x(t) \). For our specific problem, integrating the acceleration \( a(t) = 3e^{-0.2t} \) with respect to \( t \) helped us find the velocity:
\[ v(t) = \int 3e^{-0.2t} \, dt = -15e^{-0.2t} + C \]
We integrate once more to find the particle's position:
\[ x(t) = \int (-15e^{-0.2t} + 15) \, dt = 75e^{-0.2t} + 15t + C_1 \]
Integrating allows us to build functions for quantities that are built on the changes described by acceleration or velocity functions.
  • Integration is used to reverse differentiation.
  • Enables the calculation of velocity from acceleration and position from velocity.
  • Always results in an integration constant that needs to be determined with initial conditions.
Initial Conditions
Initial conditions are known values at a specific time that help solve for constants after integrating. They provide the details necessary to tailor general solutions to particular scenarios.
For our problem, initial conditions are given at \( t = 0 \) with \( v(0) = 0 \) and \( x(0) = 0 \). After integrating, these initial conditions are crucial to find the integration constants \( C \) and \( C_1 \). Applying the initial condition for velocity, we substitute into the velocity equation:
\[ 0 = -15e^0 + C \rightarrow C = 15 \]
Similarly, for the position function:
\[ 0 = 75e^0 + C_1 \rightarrow C_1 = -75 \]
Initial conditions ensure the solution fits the particular motion scenario of the problem, whether it's a starting point, velocity, or another state variable's initial value.
  • Provide specific starting points or known values for velocity and position.
  • Used to determine integration constants.
  • Make the solution unique to the given problem situation.
Velocity and Position
Velocity and position functions describe the motion details of a particle after considering its acceleration and initial conditions. The velocity function is obtained first by integrating the acceleration function.
In this case, the velocity at any time \( t \) is represented by \( v(t) = -15e^{-0.2t} + 15 \). Calculating for a specific time, \( t = 0.5 \), the velocity becomes \( v(0.5) \approx 1.428 \text{ ft/s} \).
Similarly, a second integration gives the position function \( x(t) \). In the exercise, at \( t = 0.5 \), the position is \( x(0.5) \approx 0.36 \text{ ft} \).
Together, velocity and position functions give complete information about a particle's motion relative to time.
  • Velocity is derived from acceleration and integration.
  • Position is derived from velocity through a second integration.
  • Provide insight into a particle's trajectory and timing.
  • Critical for determining exact states of motion at any time \( t \).

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Most popular questions from this chapter

A sprinter in a \(100-\mathrm{m}\) race accelerates uniformly for the first \(35 \mathrm{m}\) and then runs with constant velocity. If the sprinter's time for the first \(35 \mathrm{m}\) is \(5.4 \mathrm{s}\), determine \((a)\) his acceleration, \((b)\) his final velocity, \((c)\) his time for the race.

The acceleration of a particle is defined by the relation \(a=-k / x\) It has been experimentally determined that \(v=15\) fts when \(x=0.6 \mathrm{ft}\) and that \(v=9 \mathrm{ft} / \mathrm{s}\) when \(x=1.2\) ft. Determine (a) the velocity of the particle when \(x=1.5 \mathrm{ft},(b)\) the position of the particle at which its velocity is zero.

Determine the speed of a satellite relative to the indicated planet if the satellite is to travel indefinitely in a circular orbit \(100 \mathrm{mi}\) above the surface of the planet. (See information given in Probs. \(11.153-11.154 .)\) $$ \begin{array}{l}{11.155 \text { Venus: } g=29.20 \mathrm{ft} / \mathrm{s}^{2}, R=3761 \mathrm{mi}} \\ {11.156 \mathrm{Mars}: g=12.17 \mathrm{ft} / \mathrm{s}^{2}, R=2102 \mathrm{mi}} \\ {11.157 \text { Jupiter: } g=75.35 \mathrm{ft} / \mathrm{s}^{2}, R=44,432 \mathrm{mi}}\end{array} $$

A commuter train traveling at \(40 \mathrm{mi} / \mathrm{h}\) is \(3 \mathrm{mi}\) from a station. The train then decelerates so that its speed is \(20 \mathrm{mi} / \mathrm{h}\) when it is \(0.5 \mathrm{mi}\) from the station. Knowing that the train arrives at the station \(7.5 \mathrm{min}\) after beginning to decelerate and assuming constant decelerations, determine (a) the time required for the train to travel the first \(2.5 \mathrm{mi}\), \((b)\) the speed of the train as it arrives at the station, ( \(c\) ) the final constant deceleration of the train.

Steep safety ramps are built beside mountain highways to enable vehicles with defective brakes to stop safely. A truck enters a 750 -ft ramp at a high speed \(v_{0}\) and travels \(540 \mathrm{ft}\) in \(6 \mathrm{s}\) at constant deceleration before its speed is reduced to \(v_{0} / 2 .\) Assuming the same constant deceleration, determine ( \(a\) ) the additional time required for the truck to stop \((b)\) the additional distance traveled by the truck.

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