4.4.28 · D1Multivariable Calculus

Foundations — Fundamental theorem for line integrals

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This page assumes nothing. Every symbol the parent note (Fundamental theorem for line integrals) throws at you — , , , the dot, the integral — is built here from a blank page. Read top to bottom; each block earns the next.


0. The picture we keep returning to

Imagine a warm, hilly landscape at sunset. At every point on the ground you can ask: how high am I? That single number, height, is our first object.

Figure — Fundamental theorem for line integrals

1. A point in the plane:

  • Plain words: an address on the ground.
  • Picture: a single dot on the peach floor of the landscape.
  • Why the topic needs it: the endpoints and in are just two such addresses.

We will meet later — same idea with a third number for "up".


2. A scalar function: — the height map

  • Plain words: a machine: feed in an address, get out a height.
  • Picture: the surface of the hill — but painted as a flat map where colour = height.
  • Why the topic needs it: this is the potential function. FTLI's whole payoff is that the answer is , two readings of this machine.
Figure — Fundamental theorem for line integrals

The curved lines in that figure are contour lines (or level curves): all the addresses at the same height, exactly like on a real hiking map. Where they crowd together, the hill is steep.


3. Partial derivatives: and

Before the arrows, we need to measure steepness in one direction at a time.

  • Plain words: "If I nudge a tiny bit and freeze , how fast does the height change?"
  • Why this tool and not the ordinary derivative? An ordinary derivative needs a function of one variable. Our has two inputs. The partial derivative is the honest way to ask "change in one input only" — we simply pretend the other input is a constant.

4. The gradient: — the uphill arrow

Now we bundle both slopes into a single object that points the way up.

  • Plain words: at every point, an arrow whose direction is straight uphill and whose length is how steep the hill is there.
  • Picture: short arrows scattered over the map, all leaning toward higher ground, longest where contours crowd.
  • Why the topic needs it: FTLI is only about fields of the special form . The whole theorem is "when the field is a gradient, the integral is easy."
Figure — Fundamental theorem for line integrals

5. A vector: bold , arrows, and length

The gradient is a vector, so let us pin that word down.

  • Plain words: "go this way, this far."
  • Picture: a single arrow floating on the map.
  • Why the topic needs it: the field , the gradient , the position and the velocity are all vectors. Bold = arrow, plain = number.

6. A vector field:

  • Plain words: wind on a weather map — every spot has its own gust.
  • Picture: a whole meadow of arrows.
  • Why the topic needs it: measures how much a field "pushes you along" a path. When happens to equal , we call it conservative (see Conservative vector fields) and FTLI applies.

7. A parametrised curve:

We need to describe the trail we walk.

  • Plain words: a movie of a hiker; is the clock.
  • Picture: a curve on the map with a moving dot and a timestamp.
  • Why the topic needs it: the parent's Step 1 turns the line integral into an ordinary integral in using exactly this .

The tiny displacement in the parent note, , is just "velocity tiny time = tiny step."


8. The dot product:

The symbol between and is a dot, and it is not ordinary multiplication.

  • Plain words: big and positive when the arrows agree, zero when they are perpendicular, negative when they oppose.
  • Why this tool and not multiplication? You cannot multiply two arrows like numbers. But you can ask "how much of the field pushes me forward along my step?" That question — field component along motion — is precisely the dot product. That is why the line integrand is and not .
Figure — Fundamental theorem for line integrals

9. The integral sign: and

  • Plain words: a grand total of tiny contributions.
  • The line integral : at each tiny step along the path , take the push-along-the-step number , and total them. See Line integrals of vector fields.
  • The loop : the same, with a little circle warning you the path is closed (ends where it began).

10. The Fundamental Theorem of Calculus (the 1D ancestor)

  • Plain words: the whole equals (final value) − (starting value).
  • Why the topic needs it: FTLI is this exact statement, dressed up. The parent proof reduces the line integral to and then quotes this. See Fundamental Theorem of Calculus.

11. Putting the symbols in one sentence

Now every piece of the parent's headline formula is defined:

Read aloud: "Adding up the uphill-push along every tiny step of the trail equals the height at the end minus the height at the start."


Prerequisite map

Point x y

Scalar height f

Partial slopes f_x f_y

Gradient nabla f uphill arrow

Vector arrow

Vector field F equals P Q

Parametrised curve r of t

Velocity r prime t

Dot product

Line integral over C

Ordinary FTC

FTLI f B minus f A


Equipment checklist

Test yourself — cover the right side and answer before revealing.

What is a scalar function ?
A machine that takes a point and returns one number — here, the height of the hill.
What does the partial derivative measure?
The rate of change of as you step in the -direction, with held frozen.
What is in components, and where does it point?
; it points in the direction of steepest ascent (uphill), with length equal to the steepness.
What is a vector field ?
A rule attaching an arrow to every point of the plane.
What is and what is ?
is your position at time along a curve; is the velocity, tangent to the curve.
Compute the dot product .
.
What does the dot product tell you about two arrows?
How much they point the same way — positive if aligned, zero if perpendicular, negative if opposed.
State the ordinary Fundamental Theorem of Calculus.
: the sum of tiny changes equals the total change.
Why does equal in one line?
The integrand is the derivative of , so the 1D FTC gives .

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