Calculus II Lesson 11: Arc Length / Differential Equations Intro

  1. Upcoming
  2. Volumes
    1. Activity
  3. Arc Length
    1. Example
    2. Example
    3. Questions?
  4. Differential Equations
    1. Example
    2. Solution (if time)
  5. Overview
    1. Solutions to differential equations
    2. Order
    3. Example
    4. Solution
    5. Wrap-up

Upcoming

Volumes

More complicated regions:

Disk method over the y-axis

So we have actually 6 possible formulas:

  1. $V = \int_a^b \pi (f(x)^2) dx$.
  2. $V = \int_a^b \pi (g(y)^2) dy$.
  3. $V = \int_a^b 2\pi x f(x) dx$.
  4. $V = \int_a^b \pi (f(x)^2 - g(x)^2) dx$.
  5. $V = \int_a^b \pi (g(y)^2 - h(y)^2) dy$.
  6. $V = \int_a^b 2\pi y g(y) dy$.

Activity

Consider the following problems:

  1. Revolve the region bounded by $y = x$, $y = x^2$, $x = 0$ and $x = 1$ around the $x$-axis.
  2. Revolve the region bounded by $y = x^2$, $x = 0$, $x = 2$ and $y = 4$ around the $y$-axis.
  3. Revolve the region bounded by $y = x^2$, $x = 0$, $x = 2$ and $y = 0$ around the $y$-axis.

In small groups: For each problem:

Arc Length

Formula:

\[s = \int_a^b \sqrt{1 + (f^\prime)^2 } dx\]

First: review the notes / examples from last time.

Example

The path of a rock thrown off a 100 meter cliff (approximately) follows the curve $f(t) = 100 - 5t^2$, from $t = 0$ to $t = \sqrt{20}$ seconds. Find the length of the path the rock travels from $t = 0$ to $t = \sqrt{20}$. Round your answer to the nearest hundredth of a meter.

Example

Arc length of $f(t) = 100 - 5t^2$ from $t = 0$ to $t = \sqrt{20}$. Round your answer to the nearest hundredth of a meter.

\[\begin{align} f^\prime(x) = -10x \\ (f^\prime(x))^2 = 100x^2 \\ \int_0^{\sqrt{20}} \sqrt{1 + 100x^2}dx \end{align}\]

WolframAlpha: $\approx 100.25$ meters.

Questions?

Before we move on:

Differential Equations

Sometimes:

Example

We have a differential equation:

\[m^\prime(t) = .05 m(t)\]

What functions are proportional to their own derivatives? Exponential functions! Guess $m(t) = Ae^{kt}$, and use $m^\prime$ and $m(0)$ to find these constants $A$ and $k$.

Solution (if time)

\[\begin{align} m(t) &= Ae^{kt} \\ m^\prime(t) &= Ake^{kt} \\ &= .05 m(t) \\ &= .05 Ae^{kt} \\ k &= .05 \end{align}\]

So we have:

Find $A$?

\[\begin{align} Ae^{0} = 2 \\ A = 2 \end{align}\]

Solution:

Overview

Solutions to differential equations

Order

The order of a differential equation is the highest derivative that appears in the equation. Exercise: Identify the orders of the following:

  1. $y^\prime = y + x$
  2. $(y^\prime)^2 = (y - x)^2$
  3. $y^{\prime\prime} = -y$
  4. $y^{\prime\prime\prime} + (y^\prime)^5 = y$

We will mostly focus on first-order differential equations, but some simple higher order differential equations can be solved.

Example

A ball is thrown straight into the air with an initial velocity of 5 meters per second. It is acted on by a constant, downward force of gravity, causing an acceleration of $-9.8$ $m/s^2$.

  1. Find a formula $v(t)$ for the velocity at time $t$ seconds after the ball is thrown.
  2. How many seconds after the ball is thrown does it reach its maximum height?
  3. If the ball is thrown at a height of 2 meters above the ground, what is the maximum height reached?

Solution

Since $v^\prime(t) = a(t)$, and $a(t) = -9.8$, we know:

So: $v(t) = -9.8t + C$. Since $v(0) = 5$, we can compute $5 = -9.8(0) + C$, so $C = 5$.

So our formula for the velocity is $v(t) = -9.8t + 5$. Going back to Calc I:

Therefore $h(t) = -4.9t^2 + 5t + 2$. Then $h(\frac{5}{9.8}) \approx 3.28$ meters. This is basically the exam 1 extra credit problem.

Wrap-up