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The acceleration of a particle is given by \(a=-k s^{2}\) where \(a\) is in meters per second squared, \(k\) is a constant, and \(s\) is in meters. Determine the velocity of the particle as a function of its position \(s\). Evaluate your expression for \(s=5 \mathrm{m}\) if \(k=0.1 \mathrm{m}^{-1} \mathrm{s}^{-2}\) and the initial conditions at time \(t=0\) are \(s_{0}=3 \mathrm{m}\) and \\[ v_{0}=10 \mathrm{m} / \mathrm{s} \\]

Short Answer

Expert verified
The velocity at \(s = 5 \text{ m}\) is approximately \(9.65 \text{ m/s}\).

Step by step solution

01

Relate Acceleration and Velocity

The acceleration of a particle is given by \( a = \frac{dv}{dt} \). Using the chain rule, \( a \) can also be expressed as \( a = \frac{dv}{ds} \frac{ds}{dt} = v \frac{dv}{ds} \). Thus, we set up the equation \( v \frac{dv}{ds} = -k s^2 \).
02

Separate Variables and Integrate

We separate variables by moving \( v dv \) to one side and \( -k s^2 ds \) to the other side:\[ v dv = -k s^2 ds \]Integrate both sides:\[ \int v dv = \int -k s^2 ds \]
03

Evaluate the Integrals

Calculate the left integral:\[ \int v dv = \frac{v^2}{2} \]Now, calculate the right integral:\[ \int -k s^2 ds = -k \frac{s^3}{3} + C \]where \( C \) is the integration constant.
04

Solve for v in Terms of s

Combine the results from the integrals:\[ \frac{v^2}{2} = -k \frac{s^3}{3} + C \]Multiply through by 2 to solve for \( v^2 \):\[ v^2 = -\frac{2ks^3}{3} + 2C \]So, the velocity \( v \) can be given by:\[ v = \pm \sqrt{-\frac{2ks^3}{3} + 2C} \]
05

Use Initial Conditions to Find Constant C

Given the initial conditions at \( s_0 = 3 \text{ m} \) and \( v_0 = 10 \text{ m/s} \), substitute these into the equation:\[ 10^2 = -\frac{2k(3)^3}{3} + 2C \]Simplifying, \( 100 = -\frac{54k}{3} + 2C = -18k + 2C \). Solve for \( C \):\[ 2C = 100 + 18k \]\[ C = 50 + 9k \]
06

Substitute for k and Evaluate at s = 5 m

Substituting \( k = 0.1 \text{ m}^{-1} \text{s}^{-2} \) into \( C \):\[ C = 50 + 9(0.1) = 50.9 \]Now, substitute into the expression for \( v \):\[ v = \pm \sqrt{-\frac{2(0.1)(5)^3}{3} + 2(50.9)} \]Calculate:\[ v = \pm \sqrt{-\frac{2(0.1)(125)}{3} + 101.8} \]\[ v = \pm \sqrt{-\frac{25}{3} + 101.8} \]\[ v = \pm \sqrt{93.133} \]
07

Calculate the Final Velocity Value

Determine the value of the velocity:\[ v = \pm 9.65 \text{ m/s} \]Choose positive because particle started moving with positive velocity.

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Key Concepts

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

Particle Acceleration
Acceleration is a measure of how quickly a particle's velocity changes over time. In this exercise, the particle's acceleration depends on its position, given by the formula \( a = -k s^2 \), where \( k \) is a constant and \( s \) is the position. This kind of relationship suggests that the particle's acceleration changes with the square of the position. Such relationships are common in fields involving forces that vary with distance, like gravity or electrostatics.
In this scenario, the negative sign indicates that the acceleration is in the opposite direction to the increase in position, meaning it's acting to decelerate the particle. Solving for velocity here involves understanding how displacement affects acceleration, and then linking this with the particle's change in velocity over time.
Integration of Differential Equations
In mathematics, a differential equation relates a function to its derivatives, and integrating such equations helps us find solutions that describe the behavior of a system. Here, our task is to find the velocity as a function of position.
The given acceleration equation \( a = -k s^2 \) can be transformed using the relationship \( a = v \frac{dv}{ds} \), enabling us to express the problem as a separable differential equation. The integration becomes:
  • Move terms to separate each variable: \( v dv = -k s^2 ds \).
  • Integrate both sides: \( \int v dv = \int -k s^2 ds \).
  • After integration, these become \( \frac{v^2}{2} \) on the left and \( -\frac{ks^3}{3} + C \) for the right, where \( C \) is a constant.
These steps help determine how velocity changes with position, paving the way to solve for precise values, given initial conditions or other specific parameters.
Initial Conditions
Initial conditions are values set at the beginning of a problem that allow us to find unknown constants when solving differential equations. In this problem, the initial conditions give us specific values for position \( s_0 = 3 \text{ m} \) and velocity \( v_0 = 10 \text{ m/s} \).
When integrated, differential equations include arbitrary constants. Initial conditions help to determine these constants specifically. By plugging in the initial conditions into the integrated equation:
  • You substitute \( s_0 \) and \( v_0 \) into the expression for velocity.
  • Calculate the value of \( C \), ensuring the solution fits the real-world scenario at those starting values.
For this exercise, identifying and applying the initial conditions led to determining the integration constant \( C = 50 + 9k \). Subsequently, this value aids in evaluating the velocity function at other positions, such as at \( s = 5 \text{ m} \), to obtain the final desired result.

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Most popular questions from this chapter

The speed of a car increases uniformly with time from \(50 \mathrm{km} / \mathrm{h}\) at \(A\) to \(100 \mathrm{km} / \mathrm{h}\) at \(B\) during \(10 \mathrm{sec}\) onds. The radius of curvature of the hump at \(A\) is \(40 \mathrm{m} .\) If the magnitude of the total acceleration of the mass center of the car is the same at \(B\) as at \(A,\) compute the radius of curvature \(\rho_{B}\) of the dip in the road at \(B\). The mass center of the car is \(0.6 \mathrm{m}\) from the road.

A train which is traveling at \(80 \mathrm{mi} / \mathrm{hr}\) applies its brakes as it reaches point \(A\) and slows down with a constant deceleration. Its decreased velocity is observed to be \(60 \mathrm{mi} / \mathrm{hr}\) as it passes a point \(1 / 2 \mathrm{mi}\) beyond \(A\). A car moving at \(50 \mathrm{mi} / \mathrm{hr}\) passes point \(B\) at the same instant that the train reaches point \(A\) In an unwise effort to beat the train to the crossing, the driver "steps on the gas." Calculate the constant acceleration \(a\) that the car must have in order to beat the train to the crossing by 4 seconds and find the velocity \(v\) of the car as it reaches the crossing.

An electric motor \(M\) is used to reel in cable and hoist a bicycle into the ceiling space of a garage. Pulleys are fastened to the bicycle frame with hooks at locations \(A\) and \(B\), and the motor can reel in cable at a steady rate of 12 in./sec. At this rate, how long will it take to hoist the bicycle 5 feet into the air? Assume that the bicycle remains level.

Train \(A\) is traveling at a constant speed \(v_{A}=\) \(35 \mathrm{mi} / \mathrm{hr}\) while car \(B\) travels in a straight line along the road as shown at a constant speed \(v_{B}\). A conductor \(C\) in the train begins to walk to the rear of the train car at a constant speed of \(4 \mathrm{ft} / \mathrm{sec}\) relative to the train. If the conductor perceives car \(B\) to move directly westward at \(16 \mathrm{ft} / \mathrm{sec},\) how fast is the car traveling?

A block of mass \(m\) rests on a rough horizontal surface and is attached to a spring of stiffness \(k .\) The coefficients of both static and kinetic friction are \(\mu\) The block is displaced a distance \(x_{0}\) to the right of the unstretched position of the spring and released from rest. If the value of \(x_{0}\) is large enough, the spring force will overcome the maximum available static friction force and the block will slide toward the unstretched position of the spring with an acceleration \(a=\mu g-\frac{k}{m} x,\) where \(x\) represents the amount of stretch (or compression) in the spring at any given location in the motion. Use the values \(m=5 \mathrm{kg}, k=150 \mathrm{N} / \mathrm{m}, \mu=0.40,\) and \(x_{0}=200 \mathrm{mm}\) and determine the final spring stretch (or compression \(x_{f}\) when the block comes to a complete stop.

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