A.1 First Calculus Calculations: Simple Motion
Let's jump right in and complete a simple, key Calculus calculation drawing on what you already know: use a value and a rate at a moment to compute a small change in an everyday situation.
An everyday scenario: Driving on a straight road
Scenario 1, Simple Motion: Straight road travel at 9:00 am
Hannah is driving along a long straight road. At exactly 9:00:00 she passes the 2.0 kilometer (= 2000 meter) marker on the side of the road, and is traveling at a rate of 20 meters/second.
- What is Hannah's change in position in the following 1 second, given that she is traveling at 20 meters/second?
- What is Hannah's position at 9:00:01, after that 1 second has passed? (Remember that at 9:00:00, she was at the 2000 meter marker.)
- Can you predict, with certainty, her position 1 hour later, at 10:00:00? If so, where exactly will she be? If not, why can't you?
Solution (short version).
(a) Traveling at 20 m/s for 1 second, Hannah's position changes by 20 m.
(b) So her position at 9:00:01 is 2000 + 20 = 2020 m.
(c) We cannot predict her exact position at 10:00:00 from this alone, because her rate may change during the hour. Indeed, it's likely that it does!
This simple scenario highlights two key points:
-
If we're given information about
- (i) a function's value at a particular instant (Hannah's position at 9:00:00), and
- (ii) the function's rate of change at that instant (her rate of change of position each second),
- We cannot extend this reasoning to make a prediction very far out in the future, since we're not guaranteed that the function's rate of change (here, her speed of travel) remains the same.
Let's introduce notation that we'll use throughout Calculus to the same calculation. We use t to represent time as it continuously sweeps along. And we use
dt refers to a small change in time t
In Calculus we use dt for a small change in time. Here, taking dt = 1 second is a reasonable "small step."
We'll use s for position and write s(t) to show position as a function of time. In Scenario 1,
ds refers to a small change in position s
And we'll use ds to refer to a small change in position s. Here, the small change in position ds that happens over the small 1-second time interval dt is given by
Viewed differently, we can rearrange the same relation to see that Hannah's rate of travel is
Because a rate can change over time, we indicate the rate at a specific time using a vertical bar:
And please don't lose sight of the meaning of this abstract-looking expression
For a long time now you've been thinking of speed — the rate at which an object moves — as
Encapsulating our calculation for the small change in position ds
Using this notation we can generalize our calculation to apply to the small change in position ds that happens at any time t and occurs over the short-time-interval dt:
Let's try a quick Check Question to put these ideas to use.
Check Question 1: Hannah's travel at 9:10:00
At 9:10:00, Hannah is traveling faster than she was earlier, and her rate of travel is now
We're not going to bother doing the multiplication there, and we know this is a (perhaps too) simple question. But we want to keep our focus on using this new notation, and becoming familiar with setting up calculations like this. If it seems straightforward, great: you're getting it!
Calculus in the Real World: The next time you're on the road. . .
The preceding check question suggests a simple activity you can use to start making Calculus feel more real to you already: the next time you're in a vehicle, glance at the speedometer – which shows your rate of travel
And if you happen to be currently sitting in one place, not moving, then your
Encapsulating our calculation for position after dt has passed
Let's extend the use of our new notation to express the calculation we made to find Hannah's position 1 second after 9:00:00:
And since we're using
Check Question 2: Calvin tosses a ball
Calvin tosses a ball straight up. He starts a stopwatch the moment the ball leaves his hand, and time t represents the number of seconds that pass since that initial moment. We'll measure time in seconds, which we abbreviate "s."
Let's use y(t) to denote the ball's height above ground level as a function of time t. We'll measure the ball's height in meters, which we abbreviate "m."
At t = 0.50 s, the ball is at a height of
-
Let's set up the calculation to find the ball's height 0.01 s later,
𝑦 ( 0 . 5 1 s ) . We won't bother to complete the simple math there; instead let's focus on the Calculus ideas that are probably new to you. - At t = 0.80 s, the ball is still traveling upward but losing speed as it approaches the top of its trajectory. Let's compare the ball's rate of travel at t = 0.80 s,
to its rate at the earlier moment t = 0.50 s,𝑑 𝑦 𝑑 𝑡 ∣ a t 0 . 8 0 s , 𝑑 𝑦 𝑑 𝑡 ∣ a t 0 . 5 0 s .
The Upshot
We're on our way, doing Calculus calculations already!-
Thinking about Hannah's trip:
- ds represents the small change in an object's position s(t), and dt represents a short time interval. We write Hannah's rate of travel at 9:00:00 as
r a t e a t 9 : 0 0 : 0 0 = 𝑑 𝑠 𝑑 𝑡 ∣ a t 9 : 0 0 : 0 0 - Her tiny change in position ds over the time interval dt is then given by the familiar formulation "change = rate * time interval":
𝑑 𝑠 = ( 𝑑 𝑠 𝑑 𝑡 ∣ a t 9 : 0 0 : 0 0 ) ⋅ 𝑑 𝑡
- ds represents the small change in an object's position s(t), and dt represents a short time interval. We write Hannah's rate of travel at 9:00:00 as
- If we know an object's position
at a given moment, and its rate of travel at time t,𝑠 ( 𝑡 ) , then we can predict its location a short time-interval dt later:𝑑 𝑠 𝑑 𝑡 ∣ a t t i m e 𝑡 𝑠 ( 𝑡 + 𝑑 𝑡 ) = 𝑠 ( 𝑡 ) + 𝑑 𝑠 ⏞ ¯¯¯¯ ⏞ ¯¯¯¯ ⏞ ( r a t e a t t i m e 𝑡 ) ∗ 𝑑 𝑡 - While we can use this approach to predict position a short time dt later, we can't extend our prediction out too far without further information since the rate of travel may change.
On the next screen, we'll extend our thinking about "rates" from time-based rates to more generalized rates
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