Intuition The ONE core idea
A force acting away from a pivot doesn't just push — it twists , and the strength of that twist is called torque. Everything on the parent page is built from three raw ingredients: an arrow that says where (r ), an arrow that says how you push (F ), and a machine that combines two arrows into a twist (the cross product).
This page assumes you know nothing . Every squiggle on the parent page is unpacked here, one at a time, each one leaning on the one before it. By the end you will have earned every symbol in τ = r × F .
Definition A vector — the "arrow" quantity
A vector is a quantity that needs both a size and a direction to be complete. We draw it as an arrow : the length is the size, the way it points is the direction. We write it with a little arrow on top, like r or F .
Intuition Why we need arrows at all
"5 metres" tells you a distance but not which way . "5 metres to the right" is complete — that is a vector. A push has the same problem: "50 newtons" is useless until you say which direction you push. Rotation is all about direction, so we cannot escape arrows.
Contrast this with a scalar — a plain number with no direction , like temperature (2 0 ∘ ) or mass (3 kg ). Torque's magnitude will turn out to be a scalar, but torque itself is a vector — keep that split in mind.
Before anything can twist, we need a fixed point to twist around . Call it the pivot (also "axis" or "hinge"). Think of the exact line the door swings on.
Definition Position vector
r
r is the arrow that starts at the pivot and ends at the point where the force is applied . Its length r is the distance from pivot to that contact point.
Common mistake The classic
r trap
Feels right: "r lives at the contact point, so measure it from there." The flaw: an arrow needs a tail and a head — the tail is the pivot , the head is the contact point. Start it anywhere else and every later number is wrong.
Look at figure s02: the tail of the blue arrow sits on the hinge, the head sits on the handle. The far-off handle gives a long r ; a push near the hinge gives a short r . This length is exactly why a door opens easily at the handle.
F
F is the arrow of your push: its length F is how hard (measured in newtons , symbol N), its direction is the way you push. One newton is roughly the weight of a small apple in your hand.
Now the crucial move. A push can point any way relative to r . We measure that relationship with a single number: the ==angle θ == between the two arrows, placed tail-to-tail.
θ
θ (Greek letter "theta") is the opening between r and F when their tails are joined. θ = 0 ∘ means the push points straight out along r ; θ = 9 0 ∘ means the push is exactly sideways to r ; θ = 18 0 ∘ means the push points straight back toward the pivot.
We now ask: how much of the push actually goes "sideways"? To answer we split F into two perpendicular pieces measured against r .
Intuition Why split the force at all
Only the sideways part of a push can carry the contact point around the pivot. The part pointing along r just pulls the point toward or away from the pivot — it cannot make a circle. So we must isolate the sideways part.
To split an arrow into "along" and "across" pieces we use a right triangle — and right triangles are exactly what sin and cos describe.
Definition Sine and cosine on a right triangle
Take a right triangle with one angle θ . Then
cos θ = longest side side next to θ , sin θ = longest side side opposite θ .
They are the two ways an arrow of length F "casts a shadow": F cos θ along one direction, F sin θ along the perpendicular.
In figure s03 the pink arrow (F ⊥ = F sin θ ) is the only one that curls the point around; the yellow arrow (F ∥ = F cos θ ) just tugs along the line to the pivot.
θ , so use cos ."
Feels right: we meet cos for "components along an axis" all the time. The flaw: here we need the piece across r , and that piece is F sin θ . Check the extremes: at θ = 0 ∘ the push is straight out, no twist possible — and indeed sin 0 ∘ = 0 . Cosine would wrongly give maximum. Sin to spin.
Now the star symbol of the whole topic: the × in r × F .
a × b
The cross product is an operation that eats two vectors and produces a new vector . Its size is
∣ a × b ∣ = a b sin θ ,
and its direction is perpendicular to both input arrows.
sin θ lives inside the cross product
The cross product measures the area of the parallelogram you can build from the two arrows. Base = a , height = b sin θ (the sideways reach), so area = ab sin θ . When the arrows line up (θ = 0 ) the parallelogram collapses flat → zero area → zero twist. That is exactly the door pushed into its hinges.
This is why the parent page's τ = r F sin θ was never a guess — it is forced by the cross product's built-in sin θ . See Cross Product (Vector Algebra) to go deeper on this machine itself.
Definition Right-hand rule — reading the twist direction
Point your right hand's fingers along r , then curl them toward F . Your thumb points along τ . In flat 2D problems this thumb points either out of the page (we call this + , anticlockwise) or into the page (− , clockwise).
τ
τ (Greek "tau") is the vector the machine produces: the twist . Its length τ = r F sin θ is the twisting strength; its direction is the axis about which the twist happens.
Unit: newton-metre (N·m) — a distance (m) multiplied by a force (N).
Common mistake "N·m means torque is energy."
Feels right: energy (the joule) is also N·m. The flaw: torque is a vector with an axis; energy is a plain scalar. Same units, different creatures — never add them. Write N·m for torque, J for energy.
The parent page writes forces as ( x , y , z ) and results like 6 k ^ . Here is what those hats mean.
i ^ , j ^ , k ^
These are three arrows, each of length exactly 1 , pointing along the three axes: i ^ = right (x), j ^ = up (y), k ^ = out of the page (z). Any vector is a mix of them: ( 2 , 0 , 0 ) = 2 i ^ , meaning "2 units to the right." A hat ^ always means "length one — pure direction."
Vector: size plus direction
Position vector r from pivot
Angle theta between r and F
Split force: sin theta sideways
Direction by right hand rule
Each arrow means "you need the top box before the bottom box makes sense." Notice that everything flows down into τ — and everything flows up from the single idea of a vector.
Return to the parent whenever you want the physics story: Torque — definition & physical meaning .
Test yourself — cover the right side and answer before revealing.
A vector differs from a scalar because a vector carries a direction as well as a size; a scalar is just a number.
Where does the arrow r start and end? it starts at the pivot (axis) and ends at the point where the force is applied.
What does θ measure? the angle between
r and
F when their tails are joined.
Which force component causes rotation, and what is it? the perpendicular (sideways) component, F sin θ .
Why does sin θ appear instead of cos θ ? only the sideways part twists; at
θ = 0 ∘ the push is along
r and
sin 0 ∘ = 0 gives zero torque, correctly.
What does the cross product × produce and how big is it? a new vector perpendicular to both inputs, with size ab sin θ (the parallelogram area).
What does a hat, as in k ^ , signify? a unit vector — an arrow of length exactly 1 marking a pure direction (here, out of the page).
How do you find the direction of τ ? right-hand rule — curl fingers from
r to
F , thumb points along
τ .
The 2D coordinate formula for torque is τ z = x F y − y F x , positive meaning anticlockwise (out of page).
Torque's unit and why it isn't energy newton-metre (N·m); same units as the joule but torque is a vector, energy is a scalar.