This is Thread 3 in a series, but don't worry! This thread is self-contained.
In Thread 1, we saw applications of a mass on a spring.
We solved for its future position, at time π‘. This led to π^(ππ‘), but π is "imaginary."
The position along the ground had to be βreal,β so we sought to interpret π^(ππ‘) in terms of real numbers.
In Thread 2, we tackled the exponent ππ‘. Before simplifying, it had the form π₯+ππ¦. We placed π₯+ππ¦ at
(π₯, π¦) in the plane. Then we realized
π = 0+ π1
=> π is the unit along the y-axis, located at (0, 1)
We also found that multiplying by π amounts to rotating by +90Β°. In particular, multiplying π‘ by π yields ππ‘ on the y-axis.
So, we know what ππ‘ looks like. Now, weβll tackle π^(ππ‘) as a whole: what does π^(ππ‘) look like?
We expect π^(ππ‘) to be a "complex" number π₯+ππ¦. After all, complex numbers include all numbers we know, including π, π, and π‘.
As π‘ is the only variable in π^(ππ‘), π₯ and π¦ depend on π‘:
π^(ππ‘) = π₯(π‘)+ππ¦(π‘).
So, π^(ππ‘) is located at the point (π₯(π‘), π¦(π‘)). Since π‘ represents time, this is a moving point. What path will it take?
We could try to plot (π₯(π‘), π¦(π‘)) for many values of π‘, but we only know how to find π^(ππ‘) when the exponent is real. That only happens at t=0. Then we get
=π^(0)
=1
=1+0π.
So, (1, 0) is the initial point.
Fortunately, one point is enough!
Calculus lets us plot curves without a table of points: we calculate the direction, to anticipate where our starting point will move next.
In other words, we calculate the derivative.
Specifically,
(π₯(π‘), π¦(π‘)) is the position at time π‘
(π₯β²(π‘), π¦β²(π‘)) is the velocity, which gives the direction
How can we calculate the velocity? Our approach all along has been to calculate with π as if it's realβ¦
This is fine.
As Herodotus apparently learned from his travels in Persia, it's often a good strategy to...
deliberate while drunk,
decide while sober.
We're in the drunken discovery phase right now. If we are so inclined, we can make definitions and apply modern rigor later.
For real r, the derivative of e^(rt) is re^(rt). That is, u=e^(rt) grows exponentially, at a rate proportional to the amount: u'=ru.
So, differentiating e^(rt) amounts to multiplying by r. If we treat π the same way, differentiating e^(πt) amounts to multiplying by π.
Remember, multiplying by π causes a rotation by +90Β°. Hence, the velocity is obtained by rotating the position +90Β°.
Beautiful! Itβs so much simpler than we wouldβve initially guessed.
Can you guess the path that the moving point will follow?
Itβs a circle! The unit circle, to be precise.
Now, if only we knew formulas for a point moving around the unit circleβ¦
We know this from trigonometry:
(x(t), y(t)) = (cos(t), sin(t)).
(This assumes unit speed, but weβre safe. Each velocity vector is obtained by rotating a position vector of a point on the unit circle. Each position vector has length one, so the velocity vectors must as well.)
Weβve done it!
Weβve determined that π^(ππ‘) is located at
(cos(π‘), sin(π‘)).
It follows that
π^(ππ‘) = cos(π‘)+π sin(π‘)
This is Eulerβs formula.
Now that we understand the pieces, we can understand the entire derivation with a picture!
#MTBoS
What's your #calculus narrative? Do you have a one-sentence summary you can repeat to students throughout the course so that they absorb the main idea?
I was inspired by the attached thread to share my current best answer...
#MTBoS Has Germany caught up to the US in COVID-19 deaths? If you move from California to Wyoming, do you really have 3.6 times more voting power? The new #Eventmath wiki pairs current events with #math lesson plans to help students fight misinformation. Retweet for numeracy!
Eventmath is a free and open resource that we build together. Interested in contributing or using lesson plans? Want to be a part of the community? You can add your Twitter handle to Community Members in this Google Doc: docs.google.com/document/d/1gtβ¦
We have big plans, but we're starting with a humble Google Doc. If youβd like to make and share your first contribution now, we have a prioritized list of tasks. The smallest takes only a few seconds. Just head on over to the To-Do List in the Google Doc to make a difference!