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Further kinematics

Vectors in kinematics

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Further kinematics

Vector methods with projectiles

Variable acceleration in one dimension

Differentiating vectors

Integrating vectors

Application of forces

Static particles

Modelling with statics

Friction with static particles

Statics of rigid bodies

Dynamics and inclined planes

Connected particles

Projectiles

Horizontal projection

Projectiles: Horizontal and vertical components

Projection at any angle

Equation of the trajectory of a projectile

Forces and friction

Resolving forces

Inclined planes

The coefficient of friction

Moments

Resultant moments

Equilibrium

Centre of mass

Tilting

Laminas

Forces and motion

Force diagrams

Forces as vectors

Forces and acceleration

Motion in two dimensions

Connected particles

Pulleys

Variable acceleration

Functions of time: Displacement, velocity, acceleration

Using differentiation to find velocity and acceleration

Maxima and minima problems

Using integration to find velocity and displacement

Constant acceleration formulae

Constant acceleration

Displacement-time graphs

Velocity-time graphs

Constant acceleration: Deriving formulae

Constant acceleration formulae: SUVAT

Vertical motion under gravity

Modelling in mechanics

Modelling assumptions

Quantities and units in mechanics

Working with vectors

Normal distribution

The normal distribution

The normal distribution: Finding probabilities

The inverse normal distribution function

The standard normal distribution

Finding the mean and standard deviation

Normal approximation to the binomial distribution

Hypothesis testing with the normal distribution

Conditional probability

Set notation

Conditional probability

Conditional probability in Venn diagrams

Probability formulae

Conditional probability: Tree diagrams

Correlation and hypothesis testing

Exponential models

Measuring correlation

Hypothesis testing for zero correlation

Hypothesis testing I

Hypothesis testing

Hypothesis testing: Finding critical values

One-tailed tests

Two-tailed tests

Binomial distribution

Probability distributions

The binomial distribution

Cumulative probabilities

Probability

Calculating probabilities

Venn diagrams

Probability: Mutually exclusive and independent events

Probability: Tree diagrams

Representation of data

Outliers

Box plots

Cumulative frequency

Histograms

Comparing data sets

Correlation

Linear regression

Measures of location and spread

Measures of central tendency: Mean, median, mode

Measures of spread: Range

Variance and standard deviation

Data collection

Population and samples

Sampling techniques

Types of data

Vectors II

3D coordinates

Vectors in 3D

Solving geometric problems

Applications to mechanics: 3D vectors

Numerical methods

Locating roots

Iteration

Staircase and cobweb diagrams

Newton-Raphson method

Numerical methods: Applications to modelling

Integration II

Integrating standard functions

Integrating f(ax + b)

Integration with trigonometric identities

Reverse chain rule

Integration by substitution

Integration by parts

Integration using partial fractions

Finding areas using integration

The trapezium rule

Solving differential equations

Modelling with differential equations

Differentiation II

Differentiating sin x and cos x

Differentiating exponentials and logarithmic functions

The chain rule

The product rule

The quotient rule

Differentiating inverse functions

Differentiating trigonometric functions

Parametric differentiation

Implicit differentiation

Second derivatives: Concave and convex functions

Connected rates of change

Trigonometry and modelling

Addition formulae

Using the angle addition formulae

Double angle formulae

Solving trigonometric equations: Double angle formula

Simplifying a cos x + b sin x

Proving trigonometric identities

Modelling with trigonometric functions

Trigonometric functions

Secant, cosecant and cotangent

Graphs of sec x, cosec x and cot x

Solving equations with sec x, cosec x and cot x

Further trigonometric identities

Inverse trigonometric functions

Radians

Radian measure

Arc length

Areas of sectors and segments

Solving trigonometric equations

Small angle approximations

Sequences and series

Sequences revision

Arithmetic sequences

Arithmetic series

Geometric sequences

Geometric series

Sum to infinity

Sigma notation

Modelling with sequences and series

Binomial expansion II

Binomial expansion: (1+x)^n

Binomial expansion: (a+bx)^n

Binomial expansion with partial fractions

Binomial expansion of compound expressions

Parametric equations

Using trigonometric identities

Sketching parametric curves

Points of intersection of parametric curves

Modelling with parametric equations

Functions

Functions and mappings

Composite functions

Inverse functions

The modulus function

y = |f(x)| and y = f(|x|)

Combining transformations

Solving modulus equations

Modulus inequalities

Algebraic fractions

Operations with algebraic fractions

Partial fractions

Repeated factors

Algebraic division

Proof II

Proof by contradiction

Criticising proofs

Vectors I

Vectors

Representing vectors

Magnitude and direction of a vector

Position vectors and displacement vectors

Solving geometric problems

Modelling with vectors

Integration I

Integrating x^n

Indefinite integrals

Finding functions by integrating

Definite integrals

Area under a curve

Area under the x-axis

Area between a curve and a line

Differentiation I

Finding the gradient of a curve

Differentiation from first principles

Differentiating x^n

Differentiating functions with multiple terms

Gradients, tangents and normals

Increasing and decreasing functions

Second order derivatives

Stationary points

Sketching gradient functions

Modelling with differentiation

Exponentials and logarithms

Exponential functions

y = e^x

Exponential modelling

Logarithms

Laws of logarithms

Solving equations using logarithms

Natural logarithms

Logarithms and non-linear data

Harder exponential modelling

Trigonometric equations

Angles in all four quadrants

Exact trigonometric values

Trigonometric identities

Simple trigonometric equations

Harder trigonometric equations

Equations and identities

Trigonometry

The cosine rule

The sine rule

Area of a triangle

Solving triangle problems

Trig graphs: sin x, cos x, tan x

Transforming trigonometric graphs

Binomial expansion I

Pascal's triangle

Factorial notation

Binomial expansion

Solving binomial problems

Binomial estimation

Circles

Midpoints and perpendicular bisectors

Equation of a circle

Intersection of straight lines and circles

Using tangent and chord properties

Circles and triangles

Intersection of two circles

Straight line graphs

y = mx + c

Equations of straight lines

Parallel and perpendicular lines

Length and area

Modelling with straight lines

Transformations

Translating graphs

Stretching and reflecting graphs

Transforming graphs

Sketching graphs

Cubic graphs

Quartic graphs

Reciprocal graphs

Points of intersection

Using the discriminant

Direct and inverse proportion

Polynomials

Functions

Expanding brackets

Factorising

Simplifying algebraic fractions

Polynomial division

The factor theorem

Equations and inequalities

Linear simultaneous equations

Quadratic simultaneous equations

Set notation and interval notation

Linear inequalities

Quadratic inequalities

Inequalities on graphs

Inequality regions

Quadratics

Solving quadratic equations

Completing the square

Quadratic graphs

Identifying the discriminant

Solving disguised quadratics

Indices and surds

Laws of indices

Negative and fractional indices

Surds

Rationalising the denominator

Proof I

Mathematical structure and arguments

Disproof by counterexample

Proof by deduction

Proof by exhaustion

Explainer Video

Tutor: Meera

Summary

Vectors in kinematics

In a nutshell

Position vectors are quantities that determine the position of one point in space, always relative to another point. Vectors are useful tools used to describe motion in a plane, as they have a direction and a magnitude.

Equations

DESCRIPTION	EQUATION
Movement with constant velocity.	$\bold r = \bold r_{\bold 0} + \bold v t$
Movement with constant acceleration.	$\bold r = \bold u t + \cfrac{1}{2} \bold a t^2$ $\bold v = \bold u + \bold a t$

DESCRIPTION

EQUATION

Movement with constant velocity.

$\bold r = \bold r_{\bold 0} + \bold v t$

Movement with constant acceleration.

$\bold r = \bold u t + \cfrac{1}{2} \bold a t^2$

$\bold v = \bold u + \bold a t$

Variable definitions

Quantity name	symbol	UNIT NAME	UNIT
$Displacement \ vector$	$\bold r$	$Metres$	$m$
$Initial \ displacement \ vector$	$\bold r_0$	$Metres$	$m$
$Velocity \ vector$	$\bold v$	$Metres \ per\ second$	$ms^{-1}$
$Initial \ velocity \ vector$	$\bold u$	$Metres \ per\ second$	$ms^{-1}$
$Acceleration \ vector$	$\bold a$	$Metres\ per \ second\ squared$	$ms^{-2}$
$Time$	$t$	$Seconds$	$s$

Vectors in kinematics

PROCEDURE

1.	Identify the variables and data in the question.
2.	Recall the relevant equations of motion.
3.	Group the terms according to the unit vectors $\bold i$ and $\bold j$ , which are unit vectors often defined to be due east and north respectively.

Example 1

A particle starts from the point with position vector $(5\bold{i} + 10 \bold{j}) \ m$ and moves with constant velocity $(2\bold{i} - 2 \bold{j})\ ms^{-1}$ .

i) Find the position vector of this particle after $10$ seconds.

ii) Show that the particle is never at the point $(0,0).$

i) Find the position vector of this particle after $10$ seconds.

Using the equation $\bold r = \bold r_0 + \bold vt$ , substitute $\bold r_0 =(5\bold{i} + 10 \bold{j})\, m$ and $\bold v=(2\bold{i} - 2 \bold{j})\ ms^{-1}$ :

$\bold r = \bold r_0 + \bold v t = \left[(5\bold i + 10 \bold{j}) +(2\bold{i} - 2 \bold{j})t\right] \ m$ 

Group the terms according to the unit vectors:

 $\bold r = \left[(5+2t)\bold{i} +(10-2t)\bold j\right]\ m$ 

Now substitute the value of the time $t=10 \ s$ :

$\begin{aligned}\bold r &= (5+2\times 10)\bold{i} +(10-2\times 10)\bold j \\&=(5+20)\bold{i} +(10-20)\bold j \\&= (25\bold{i} -10\bold j) \ m\end{aligned}$

In conclusion, $\underline{\bold r = (25 \bold i - 10 \bold j) \ m}$ .

ii) Show that the particle is never at the point $(0,0).$

Using $\bold r = \left[(5+2t)\bold{i} +(10-2t)\bold j\right]m$ (from the first part), you only have to substitute $\bold r = (0 \bold i + 0 \bold j) \ m$ . Therefore:

$\bold r = 0\bold i + 0 \bold j = (5+2t)\bold{i} +(10-2t)\bold j\implies\begin{cases}0 \bold i = (5 +2t)\bold i \\0 \bold j = (10 -2 t )\bold j\end{cases} \implies \begin{cases}t=-0.4 \ s\\t = 5 \ s\end{cases}$

The particle is never at the origin because the two times are not consistent.

Example 2

A particle $P$ initially moves with velocity $(3\bold i - 8\bold j)\ ms^{-1}$ . It has an acceleration of $(-2 \bold i + 3 \bold j) \ ms^{-2}$ .

i) Find the velocity of $P$ after $t=3 \ s.$ 

ii) Find the speed of $P$ at $t = 3 \ s$ to $2\space d.p.$ 

i) Find the velocity of $P$ after $t=3 \ s.$ 

Using the equation $\bold v=\bold u +\bold a t$ you have to substitute $\bold u =(3\bold i - 8\bold j)\ ms^{-1}$ and $\bold a=(-2 \bold i + 3 \bold j) \ ms^{-2}$ . Therefore:

$\bold v = \left[(3\bold i - 8 \bold j) + (-2 \bold i + 3 \bold j)t\right]\ ms^{-1}$

Group the terms according to the unit vectors.

$\bold v = \left[(3 - 2t)\bold i + (-8 + 3t)\bold j\right] \ ms^{-1}$ 

Now substitute the value of the time $t = 3 \ s:$ 

$\begin{aligned}\bold v &= (3 - 2\times 3)\bold i + (-8 + 3\times 3)\bold j \\&=(3 -6)\bold i + (-8 + 9)\bold j \\&= (-3\bold i + \bold j) \ ms^{-1}\end{aligned}$ 

In conclusion $\underline{\bold v = (-3 \bold i +\bold j) \ ms^{-1}}$ 

ii) Find the speed of $P$ at $t = 3 \ s.$

The formula for speed is $\sqrt{v_x^2 + v_y^2}$ , therefore the speed of $P$ is:

$Speed \ of \ P = \sqrt{(-3)^2 +1^2 }=\sqrt{9+ 1}=\sqrt{10} = \underline{3.16 \ ms^{-1} \ (2 \ d.p.)}$ 

Learn with Basics

Length:

Unit 1

Resolving forces

Unit 2

Resolving vectors

Jump Ahead

Optional

Unit 3

Vectors in kinematics

Final Test

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FAQs - Frequently Asked Questions

Are velocity and time vectors?

Velocity is a vector, as it has a direction and a magnitude. Meanwhile, time is not a vector, as it only has a magnitude.

How is a vector defined?

A vector is defined through two features: their direction and their magnitude.

What is a vector?

A vector is a quantity that has magnitude and direction.

Vectors in kinematics

Videos

Summary

Exercises

Select Lesson

Exam Board

Further kinematics

Application of forces

Projectiles

Forces and friction

Moments

Forces and motion

Variable acceleration

Constant acceleration

Modelling in mechanics

Normal distribution

Conditional probability

Correlation and hypothesis testing

Hypothesis testing I

Binomial distribution

Probability

Representation of data

Measures of location and spread

Data collection

Vectors II

Numerical methods

Integration II

Differentiation II

Trigonometry and modelling

Trigonometric functions

Radians

Sequences and series

Binomial expansion II

Parametric equations

Functions

Algebraic fractions

Proof II

Vectors I

Integration I

Differentiation I

Exponentials and logarithms

Trigonometric equations

Trigonometry

Binomial expansion I

Circles

Straight line graphs

Transformations

Sketching graphs

Polynomials

Equations and inequalities

Quadratics

Indices and surds

Proof I

Explainer Video

Summary

​​Vectors in kinematics

​​In a nutshell

Equations

DESCRIPTION

EQUATION

Variable definitions

Quantity name

symbol

UNIT NAME

UNIT

Vectors in kinematics

PROCEDURE

Example 1

Example 2

Learn with Basics

Unit 1

Resolving forces

Unit 2

Resolving vectors

Jump Ahead

Unit 3

Vectors in kinematics

Final Test

FAQs - Frequently Asked Questions

Are velocity and time vectors?

Vectors in kinematics

In a nutshell

Vectors in kinematics

In a nutshell