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Constant acceleration Suppose that the velocity of a falling body is \(v=k \sqrt{s} \mathrm{m} / \mathrm{sec}(k\) a constant) at the instant the body has fallen \(s \mathrm{m}\) from its starting point. Show that the body's acceleration is constant.

Short Answer

Expert verified
The body's acceleration is constant and given by \( a = \frac{k^2}{2} \).

Step by step solution

01

Express Velocity in Terms of Displacement

We start with the given velocity equation: \( v = k \sqrt{s} \). This expresses the velocity \( v \) of the body as a function of the displacement \( s \).
02

Differentiate Velocity with Respect to Displacement

To find acceleration, we need the derivative of velocity with respect to time. First, differentiate the velocity expression \( v = k \sqrt{s} \) with respect to \( s \): \( \frac{dv}{ds} = \frac{k}{2\sqrt{s}} \).
03

Chain Rule Application

Use the chain rule \( \frac{dv}{dt} = \frac{dv}{ds} \cdot \frac{ds}{dt} \). Here, \( \frac{ds}{dt} = v = k \sqrt{s} \). Substitute this into the chain rule equation: \( \frac{dv}{dt} = \frac{k}{2\sqrt{s}} \cdot k \sqrt{s} \).
04

Simplify the Expression for Acceleration

Simplify the expression from the chain rule: \( \frac{dv}{dt} = \frac{k^2}{2} \). Now we see that \( \frac{dv}{dt} \), which is the acceleration \( a \), equals a constant \( \frac{k^2}{2} \).
05

Conclusion on Constant Acceleration

Thus, the body's acceleration \( a = \frac{k^2}{2} \) is a constant, since it does not depend on either \( s \) or \( t \).

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Key Concepts

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

Velocity and Displacement
In physics, understanding the relationship between velocity and displacement is essential for analyzing motion. When an object is in motion, its velocity describes how quickly it moves, while displacement is the distance it covers in a particular direction from its starting point.

In this exercise, we have the velocity of a falling body represented as a function of its displacement: \( v = k \sqrt{s} \). Here, \( v \) represents velocity, \( k \) is a constant specific to the problem, and \( s \) indicates displacement in meters. This expression shows that as the displacement increases, the velocity changes consistently with the square root of the displacement.

Key takeaways include:
  • Velocity depends on how far the object has fallen (\( s \)).
  • The constant \( k \) plays a crucial role in determining the rate of increase in velocity with respect to displacement.
  • Understanding this relation helps in determining other motion properties like acceleration.
Chain Rule in Calculus
To delve deeper into motion, we often need to link different rates of change. This is where the chain rule in calculus becomes vital. The chain rule allows us to differentiate composite functions, essentially letting us "chain" together the effect of different variables.

In this problem, the velocity \( v = k \sqrt{s} \) is differentiated with respect to time \( t \) to find acceleration, but it is only a function of displacement \( s \).

To solve this, we apply the chain rule formula:
  • The formula is \( \frac{dv}{dt} = \frac{dv}{ds} \cdot \frac{ds}{dt} \).
  • \( \frac{dv}{ds} \) is computed directly from differentiating the given velocity expression with respect to \( s \).
  • \( \frac{ds}{dt} \) is simply the velocity \( v \), giving us a way to incorporate the effect of time indirectly through displacement.
Once we have these pieces, they can be multiplied to find \( \frac{dv}{dt} \), showing the acceleration.
Differentiation
Differentiation is a fundamental concept in calculus that helps us find how functions change. It involves calculating derivatives, which gives us the rate at which a quantity changes with another quantity.

In this exercise, differentiating is used to convert the velocity function into an acceleration function. Let's break it down:
  • We start with velocity: \( v = k \sqrt{s} \).
  • When differentiating \( v \) with respect to \( s \), the formula \( \frac{dv}{ds} = \frac{k}{2\sqrt{s}} \) is obtained.
  • This represents how velocity changes as displacement changes.
Next, apply this result using the chain rule, which includes combining it with \( \frac{ds}{dt} = v \). The simplifying process results in a constant acceleration \( \frac{dv}{dt} = \frac{k^2}{2} \). Differentiation here helps translate the changing displacement directly into the acceleration, showcasing its versatility in analyzing motion.

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Most popular questions from this chapter

Suppose that the functions \(f\) and \(g\) and their derivatives with respect to \(x\) have the following values at \(x=0\) and \(x=1 .\) $$\begin{array}{|c|c|c|c|}\hline x & {f(x)} & {g(x)} & {f^{\prime}(x)} & {g^{\prime}(x)} \\ \hline 0 & {1} & {1} & {5} & {1 / 3} \\ \hline 1 & {3} & {-4} & {-1 / 3} & {-8 / 3} \\ \hline\end{array}$$ Find the derivatives with respect to \(x\) of the following combinations at the given value of \(x .\) $$\begin{array}{ll}{\text { a. } 5 f(x)-g(x),} & {x=1 \quad \text { b. } f(x) g^{3}(x), \quad x=0} \\ {\text { c. } \frac{f(x)}{g(x)+1}, \quad x=1} & {\text { d. } f(g(x)), \quad x=0}\end{array}$$ $$\begin{array}{l}{\text { e. } g(f(x)), \quad x=0 \quad \text { f. }\left(x^{11}+f(x)\right)^{-2}, \quad x=1} \\ {\text { g. } f(x+g(x)), \quad x=0}\end{array}$$

Area The area \(A\) of a triangle with sides of lengths \(a\) and \(b\) enclosing an angle of measure \(\theta\) is $$A=\frac{1}{2} a b \sin \theta.$$ a. How is \(d A / d t\) related to \(d \theta / d t\) if \(a\) and \(b\) are constant? b. How is \(d A / d t\) related to \(d \theta / d t\) and \(d a / d t\) if only \(b\) is constant? c. How is \(d A / d t\) related to \(d \theta / d t, d a / d t,\) and \(d b / d t\) if none of \(a, b,\) and \(\theta\) are constant?

The radius of an inflating balloon A spherical balloon is inflated with helium at the rate of 100\(\pi \mathrm{ft}^{3} / \mathrm{min}\) . How fast is the balloon's radius increasing at the instant the radius is 5 \(\mathrm{ft} ?\) How fast is the surface area increasing?

A growing sand pile Sand falls from a conveyor belt at the rate of 10 \(\mathrm{m}^{3} / \mathrm{min}\) onto the top of a conical pile. The height of the pile is always three-eighths of the base diameter. How fast are the (a) height and (b) radius changing when the pile is 4 \(\mathrm{m}\) high? Answer in centimeters per minute.

Particle acceleration A particle moves along the \(x\) -axis with velocity \(d x / d t=f(x) .\) Show that the particle's acceleration is \(f(x) f^{\prime}(x)\) .

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