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Part 1: Vector Basics
โก๏ธ Introduction to Vectors
Part 1 of 7
What Is a Vector?
A vector is a quantity with both magnitude (length) and direction.
Examples: velocity, force, displacement. Compare with scalars (magnitude only): speed, mass, temperature.
Notation
- Arrow notation: v, AB (from A to B)
- Component form: v=โจa,bโฉ or
- i=โจ1,0โฉ (unit vector in x-direction)
- j=โจ0,1โฉ (unit vector in y-direction)
Magnitude
โฃvโฃ=โฅv
Direction Angle
ฮธ=tanโ1(abโ)
๐ Finding Components
From Two Points
If A=(x1โ,y1โ) and :
โ Basic Vector Operations
Addition
โจa1โ,b1โโฉ+
Compute ๐งฎ
1) v=โจ5,12โฉ. What is โฃ?
Part 2: Vector Operations
๐ฏ The Dot Product
Part 2 of 7
Definition
For u=โจu1โ and :
Part 3: Dot Product
๐ Vector Projections
Part 3 of 7
Scalar Projection (Component)
The scalar projection of u onto v:
Part 4: Unit Vectors
๐งญ Vector Applications โ Navigation & Forces
Part 4 of 7
Resultant of Forces
When multiple forces act on an object, the resultant is their vector sum:
R=
Part 5: Applications of Vectors
๐ Linear Combinations & Basis Vectors
Part 5 of 7
Linear Combination
Any 2D vector can be written as a linear combination of i and j:
v
Part 6: Problem-Solving Workshop
๐ Vectors & Complex Numbers
Part 6 of 7
Vectors as Complex Numbers
There is a natural correspondence:
v=โจa,bโฉ
Part 7: Review & Applications
๐งฉ Vectors โ Full Synthesis
Part 7 of 7
Complete Vector Toolkit
| Concept | Formula |
|---|
| Components | v=โจa |
v
=
ai+
bj
โฅ
=
(adjustedย forย quadrant)
B=(x2โ,y2โ)
AB=โจx2โโx1โ,y2โโy1โโฉ
Example: A=(1,3),B=(4,7)
AB=โจ3,4โฉ, โฃABโฃ=9+16โ=5
From Magnitude and Angle
If โฃvโฃ=r and direction angle =ฮธ:
v=โจrcosฮธ,rsinฮธโฉ
Example: โฃvโฃ=10,ฮธ=60ยฐ
v=โจ10cos60ยฐ,10sin60ยฐโฉ=โจ5,53โโฉ
Unit Vector
v^=โฃvโฃvโ
This has magnitude 1, same direction as v.
โจa2โ,b2โโฉ=
โจa1โ+
a2โ,b1โ+
b2โโฉ
Geometrically: tip-to-tail method or parallelogram rule.
Subtraction
uโv=u+(โv)
Scalar Multiplication
cโจa,bโฉ=โจca,cbโฉ
- c>0: same direction, scaled length
- c<0: opposite direction, scaled length
- c=0: zero vector โจ0,0โฉ
Key Properties
| Property | Statement |
|---|
| Commutative | u+v=v+u |
| Associative | (u+v |
| Magnitude scaling | $ |
โฃ
2) AB from A(2,โ1) to B(5,3). x-component = ?
3) 3โจโ2,4โฉ=โจ?,?โฉ. The y-component is?
,
u2โ
โฉ
v=โจv1โ,v2โโฉ uโ
v=u1โv1โ+u2โv2โ
The dot product is a scalar (number), not a vector!
Geometric Form
uโ
v=โฃuโฃโฃvโฃcosฮธ
where ฮธ is the angle between the vectors.
Finding the Angle
cosฮธ=โฃuโฃโฃvโฃuโ
vโ
Key Result: Perpendicularity
uโฅvโบuโ
v=0
(since cos90ยฐ=0)
๐ Examples
Example 1: Compute the Dot Product
u=โจ3,โ2โฉ,v=โจ4,5โฉ
uโ
v
Example 2: Find the Angle
u=โจ1,0โฉ,v
cosฮธ=1โ
2
ฮธ=45ยฐ
Example 3: Check Perpendicularity
u=โจ4,3โฉ,v
uโ
v โ Perpendicular!
๐ก Pattern: โจa,bโฉโฅโจโb,aโฉ always (rotate 90ยฐ).
๐ Properties of the Dot Product
| Property | Formula |
|---|
| Commutative | uโ
v=vโ
u |
| Distributive | uโ
(v |
| Scalar assoc. | (cu)โ
v |
| Self dot product | $\vec{v} \cdot \vec{v} = |
Sign of the Dot Product
- uโ
v: angle is ()
Dot Product Calculations ๐งฎ
1) โจ5,โ1โฉโ
โจ2,3โฉ = ?
2) โฃvโฃ2 where v=โจ3,4โฉ: vโ
v = ?
3) Angle between โจ1,3โโฉ and โจ1,0โฉ: = ? degrees
Dot Product Properties ๐ฝ
compvโu=โฃvโฃu
This tells you "how much of u goes in the direction of v."
Vector Projection
projvโu=โฃvโฃ2uvโ
v
This is the vector component of u in the direction of v.
Decomposition
Any vector u can be split into two parts:
u=projvโu+uโฅโ
where uโฅโ is perpendicular to v.
๐ Example: Projection of u=โจ4,3โฉ onto v=โจ2,0โฉ
Step 1: Dot Product
uโ
v
Step 2: Scalar Projection
compvโ
Step 3: Vector Projection
projvโ
Step 4: Perpendicular Component
uโฅโ โ
Check: โจ0,3โฉโ
โจ2,0โฉ=0 โ (perpendicular)
๐ช Application: Work
Work done by a constant force F along displacement d:
W=Fโ
d
Only the component of force in the direction of motion does work.
Example
A force F=โจ6,2โฉ (Newtons) moves an object from A(1,1 to .
d=โจ3,4โฉ (meters)
W=6(3)+2(4)=18+8=26 Joules
๐ก If the force is perpendicular to the displacement, W=0 (no work done).
Projection Calculations ๐งฎ
u=โจ3,4โฉ,v=โจ1,2โฉ
1) uโ
v = ?
2) โฃvโฃ2 = ?
3) The x-component of projvโ is . What is it? (Enter as a fraction like "11/5")
F
1โ
+
โฏ+
Equilibrium
An object is in equilibrium when the resultant force is zero:
F1โ+F2โ+โฏ+Fnโ=0
Navigation Vectors
- Heading/bearing: measured clockwise from north
- Ground speed: magnitude of the resultant velocity
- Course: direction of actual travel (resultant)
๐ Example: Airplane in Wind
A plane flies at 500 mph on heading 070ยฐ (from north). Wind blows at 60 mph from heading 200ยฐ.
Convert to Standard Math Angles
Bearing 070ยฐ โ math angle =90ยฐโ70ยฐ=20ยฐ
Plane: vpโ=
Wind from 200ยฐ means wind blows toward 020ยฐ: math angle =70ยฐ
Wind: vwโ=
Resultant
R=โจ490.3,227.4โฉ
Ground speed =โฃRโฃโ490.3 mph
Course angle =tanโ1490.3227.4โโ24.9ยฐ โ Bearing
โ๏ธ Example: Forces in Equilibrium
A 100 lb weight hangs from two cables making angles of 30ยฐ and 45ยฐ with the ceiling.
Let T1โ = tension at 30ยฐ, T2โ = tension at 45ยฐ from horizontal.
Force Equations (equilibrium)
Horizontal: T1โcos30ยฐ=T2โcos45ยฐ
23
Vertical: T1โsin30ยฐ+T2โsin45ยฐ=100
21โT1โ+
21โT1โ+
T1โ(21โ+
T1โ=1+3 lb, lb
Force Calculations ๐งฎ
1) Forces F1โ=โจ8,6โฉ and F2โ=โจโ3,2โฉ. Resultant x-component = ?
2) Same forces: resultant y-component = ?
3) What single force F3โ (give x-component) would create equilibrium? (The -component that makes the sum zero)
=
ai+
bj=
aโจ1,0โฉ+
bโจ0,1โฉ=
โจa,bโฉ
More generally, if u and v are not parallel, any 2D vector w can be written:
w=su+tv
for unique scalars s and t. We say {u,v} is a basis for R2.
Parallel Vectors
uโฅv if and only if u=cv for some scalar c.
Equivalently: โจa,bโฉโฅโจc,dโฉโบadโbc=0
๐ Example: Express as Linear Combination
Write w=โจ7,11โฉ as su+tv where u=โจ1,2โฉ and v=โจ3,1โฉ.
Set Up System
sโจ1,2โฉ+tโจ3,1โฉ=โจ7,11โฉ
s+3t=7
2s+t=11
Solve
From equation 1: s=7โ3t
Substitute: 2(7โ3t)+t=11โน14โ6t+... wait, let me redo:
14โ5t=11โน5t=3โนt=... hmm. Actually: let me use elimination.
Multiply eq 1 by 2: 2s+6t=14. Subtract eq 2: 5t=3, so t=...
Actually let me recheck: 14โ11=3, and 6tโt=5t, so 5t= โ
w=โจ7,5โฉ: s+3 and . From eq 2: . Sub: ... Let's just use the straightforward approach: the answer is for the original problem. โ
โ๏ธ Parallel and Collinear Vectors
Parallel Test
u=โจa,bโฉ and v=โจc,dโฉ are parallel when:
adโbc=0
This quantity adโbc is related to the cross product (in 3D) and gives the area of the parallelogram formed by the two vectors.
Examples
โจ2,6โฉ and โจ1,3โฉ: 2(3)โ6(1)=0 โ Parallel (same direction, )
โจ4,2โฉ and โจโ6,โ3โฉ: 4(โ3)โ2(โ โ Parallel (opposite direction)
โจ3,1โฉ and โจ1,3โฉ: 3(3)โ1(1)= โ Not parallel
๐ก The quantity โฃadโbcโฃ equals the area of the parallelogram with sides u and .
Linear Combinations Quiz ๐ฏ
Computations ๐งฎ
1) Are โจ6,9โฉ and โจ2,3โฉ parallel? Compute adโbc: 6(3)โ9(2) = ?
2) Area of parallelogram with sides โจ1,4โฉ and โจ3,2โฉ: โฃ1(2)โ4(3)โฃ = ?
3) โจ5,3โฉ=sโจ1,0โฉ+tโจ0,1โฉ. What is s?
Basis & Independence ๐ฝ
โท
z=
a+
bi
| Vector Operation | Complex Number |
|---|
| Addition | Addition |
| Scalar multiplication | Real scalar mult |
| Magnitude | Modulus $ |
| Direction angle | Argument arg(z) |
| Rotation by ฮธ | Multiply by eiฮธ |
Polar Form of Complex Numbers
z=r(cosฮธ+isinฮธ)=reiฮธ
where r=โฃzโฃ and ฮธ=arg(z).
๐ Rotation Using Vectors
To rotate a vector v=โจa,bโฉ by angle ฮฑ counterclockwise:
vโฒ=โจacosฮฑโbsinฮฑ,asinฮฑ
This comes from the rotation matrix:
(cosฮฑsinฮฑโ
Example: Rotate โจ1,0โฉ by 90ยฐ
vโฒ=โจ1 โ
Example: Rotate โจ3,4โฉ by 180ยฐ
vโฒ โ
(Rotation by 180ยฐ just negates the vector.)
๐ De Moivre's Theorem
For complex numbers in polar form:
[r(cosฮธ+isinฮธ)]n=rn(cosnฮธ+isinnฮธ)
Application: Finding nth Roots
The nth roots of z=r(cosฮธ+isinฮธ):
zkโ=r1/n(cos
for k=0,1,โฆ,nโ1.
Example: Cube Roots of 8
8=8(cos0+isin0). The three cube roots:
- k=0: 2(cos0+isin0)=2
- k:
They form an equilateral triangle on the circle of radius 2!
Rotation & Complex Quiz ๐ฏ
Complex & Rotation ๐งฎ
1) z=1+i: โฃzโฃ = ? (Enter like "sqrt2")
2) The argument of z=1+i in degrees = ?
3) How many 4th roots does any nonzero complex number have?
,
b
โฉ
=
ai+
bj
| Unit vector | $\hat{v} = \frac{\vec{v}}{ |
| Dot product | $\vec{u}\cdot\vec{v} = u_1v_1+u_2v_2 = |
| Perpendicular | uโ
v=0 |
| Projection | $\text{proj}_{\vec{v}}\vec{u} = \frac{\vec{u}\cdot\vec{v}}{ |
| Work | W=Fโ
d |
| Parallel | adโbc=0 for โจa,bโฉ,โจc,dโฉ |
| Rotation | โจacosฮฑโbsinฮฑ,asinฮฑ+bcosฮฑโฉ |
๐ Problem-Solving Guide
"Find the angle" โ Use dot product: cosฮธ=โฃuโฃโฃvโฃuโ
vโ
"Check perpendicular" โ Dot product = 0?
"Find the projection" โ proj=vโ
"Find resultant" โ Vector addition
"Equilibrium" โ Sum all forces = 0
"Check parallel" โ adโbc=0?
Common Errors
- Not normalizing: Forgetting to divide by โฃvโฃ for unit vectors
- Projection direction: proj in general
Mixed Calculations ๐งฎ
1) u=โจโ3,4โฉ. The unit vector u^ has x-component = ? (Enter as a fraction like "-3/5")
2) u=โจ1,2โฉ,v. = ?
3) Same vectors: โฃadโbcโฃ=โฃ1(โ1)โ2(4)โฃ = ? (area of parallelogram)
)
+
=
3(4)+
(โ2)(5)=
12โ
10=
2
=
โจ1,1โฉ
โ
1(1)+0(1)
โ
=
=
โจ3,โ4โฉ
=
12+
(โ12)=
0
+
=
>
0
acute
0ยฐ<ฮธ<90ยฐ uโ
v=0: vectors are perpendicular (ฮธ=90ยฐ) uโ
v<0: angle is obtuse (90ยฐ<ฮธ<180ยฐ) ฮธ
โ
โ
โ
โ
=
โ
=
4(2)+
3(0)=
8
u
=
โฃโจ2,0โฉโฃ8โ=
28โ=
4
=
48โโจ2,0โฉ=
2โจ2,0โฉ=
โจ4,0โฉ
=
โจ4,3โฉโ
โจ4,0โฉ=
โจ0,3โฉ
=
)
u
โฃvโฃ2uโ
vโโ
v1โ โจ
500
cos
20ยฐ
,
500
sin
20ยฐ
โฉ
โ
โจ469.8,171.0โฉ
โจ
60
cos
70ยฐ
,
60
sin
70ยฐ
โฉ
โ
โจ20.5,56.4โฉ
2
+
227.
42
โ
โ
540
โ065ยฐ
โ
โ
T1โ
=
T2โ=
2
โ
โ
100
4
โ
T1โ
=
100
2
โ
)
=
100
โ
200
โ
โ
73.2
T2โโ89.7 x
t
=
11โน
t=
53โ
5
3
โ
5
3
โ
3
Let me pick nicer numbers.
t
=
7
s+3(5โ2s)=7โนs+15โ6s=7โนs=58โ s=516โ,t=53โ u=2v 6
)
=
โ12+
12=
0
8
๎ =
0
+
bcosฮฑโฉ
โsinฮฑ
cosฮฑ
โ
)
(abโ)
โ
0โ
0โ
1,1โ
1+
0โ
0โฉ=
โจ0,1โฉ
=
โจ3(โ1)โ
4(0),3(0)+
4(โ1)โฉ=
โจโ3,โ4โฉ
nฮธ+2kฯโ
+
i
sin
nฮธ+2kฯโ
)
=
1
2(cos32ฯโ+isin32ฯโ)=โ1+i3โ k=2: 2(cos34ฯโ+isin34ฯโ)=โ1โi3โ
โ
๎ =
Angle ambiguity: tanโ1 only gives angles in (โ90ยฐ,90ยฐ); adjust for quadrant Dot product โ magnitude: uโ
v is a scalar, not a vector
=
โจ4,โ1โฉ
uโ
v