Pure Maths With Mechanics

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Chapter 01
Vectors and Operations

Tutor:    Dr. Fritz S.

This Lesson covers vector addition, subtraction, dot and cross product, resolution of vectors, tutorials

Chapter 02
Forces and Resolution

Tutor:    Dr. Fritz S.

Lesson covers resolution of forces into cartesian components, resultant forces, tutorials, quiz

Chapter 03
Moments of Forces

Tutor:    Dr. Fritz S.

This Lesson covers scalar and vector moments of forces and their aplications, tutorials and quiz

Chapter 04
Frictional Forces

Tutor:    Dr. Fritz S.

This Lesson covers friction, the coefficient of friction, relation with normal reaction, Applications and quiz

Chapter 05
Statics: Equilibrium of Rigid Bodies

Tutor:    Dr. Fritz S.

This Lesson covers equilibrium of collinear forces, coplanar forces, equilibriant force and some priciples

Chapter 06
Vector Calculus

Tutor:    Dr. Fritz S.

This Lesson covers differentiation and integration of vectors related to velocity and acceleartion at time, t

Chapter 07
Equations of Motion

Tutor:    Dr. Fritz S.

This Lesson is on equations of motion at constant acceleration. Parameters {u, v, s, a, t, h} e.g v=u+at

Chapter 08
Newton's Laws of Motion

Tutor:    Dr. Fritz S.

This Lesson covers Newton's 1st, 2nd and 3rd laws (Momentum, Impulse, Action/ Reaction) and Tutorials

Chapter 09
Momentum and Collisions

Tutor:    Dr. Fritz S.

This Lesson covers elastic and inelastic collisions, Newton's experimental law of impact . . .

Chapter 10
Free Fall

Tutor:    Dr. Fritz S.

This Lesson covers equations of motion for freely falling body, bounce and rebounce, graph, etc.

Chapter 11
Projectiles

Tutor:    Dr. Fritz S.

Lesson is on projectile motion, time of flight, maxi height, range, vertical/ horizontal motion

Chapter 12
Inclined Planes

Tutor:    Dr. Fritz S.

This Lesson covers statics and motion of bodies on rough/ smooth inclined planes, weight components

Chapter 13
Tension: Connected Particles

Tutor:    Dr. Fritz S.

lesson covers Tension in strings, elastic and inelastic strings, Hook's law, connected particles

Chapter 14
Centroids: Center of Gravity

Tutor:    Dr. Fritz S.

This Lesson covers finding the center of mass/gravity of uniform and non-uniform lamina, quiz, ...

Chapter 15
Vector Differential Equations

Tutor:    Dr. Fritz S.

This Lesson covers solutions to vector differential equations of particles in motion, integral limits

Chapter 16
Work, Power and Energy

Tutor:    Dr. Fritz S.

This Lesson covers work energy and power for bodies in motion, connected particles and on inclined planes

Chapter XX
Model Exam Papers and Answers

Tutor:    Dr. Fritz S.

This Lesson comprises of Model Exam papers and Answers

Chapter 01: Vectore Math - Mechanics

Tutorial 01 Rev Notes
Revision 2 1.1 Definition of Vectors
A vector quantity has both magnitude and direction. Acceleration, velocity, force and displacement are all examples of vector quantities. A scalar quantity is has only magnitude (so the direction is not important). Examples include speed, time and distance.
1.2 Components of Vectors

The process of a splitting a vector is called resolution of a vector. In simpler language it would mean, determining the effect of a vector in a particular direction. The parts of the vector obtained after splitting the vector are known as Components of the Vector.

Rectangular components of a vector: If the components of a given vector are perpendicular to each other, they are called as Rectangular components. The figure illustrates a vector A represented by OP Through the point, O two mutually perpendicular axis X and Y are drawn. From the point P, two perpendicular, PN and PM are dropped on X and Y axis respectively.


Rectangular Components
The vector Ax is the resolved part of A along the X – axis. It also known as the X-component of A and is the projection of the vector A on X- axis. Similarly, Ay is the resolved part of the A along the Y – axis, and is therefore, known as the Y – component of A
.

Applying the law of triangle of vectors to ONP, OP = ON + NP or A = Ax + Ay which also confirm that Ax, Ay are the components of A.

Moreover, in the right – angled MONP,

cosθ = Ax/A

⇒ Ax = A cosθ … (1)

Rectangular Components

sinθ = Ay/A

⇒ Ax = A sinθ … (2)

Squaring and adding equations (1) and (2) we get,

Ax² + Ay² = A² cos²θ + A² sin²θ = A² (cos²θ + sin²θ)

But, cos²θ + sin²θ = 1

∴ Ax² + Ay² = A²

⇒ A² = Ax² + Ay²

|A| = sqrt{Ax² + Ay²}

This equation gives the magnitude of the given vector in terms of the magnitudes of the components of the given vector.

In the figure, the velocity vector V is represented by the vector OP. Resolving V into its two rectangular components, we have V = Vxi + Vxj. In terms of the unit vectors i, j, V = Vxi + Vxj

Where,

Vx = V cosθ, Vy = V sinθ and tanθ = Vy/ Vx

How to find the Resolution of Vectors?

Example 01: The Diagram above shows two forces of magnitude 25N are acting on an object of mass 2kg. Find the acceleration of object, in m/s².

Resolution of Vectors

Solution: Given,

Mass (m) = 2kg

Horizontal component of the forces = 25 cos 45° + 25 cos 45° = 35.36 N

Vertical component of the forces = 25 cos 45° – 25 cos 45° = 0 N

The acceleration of the object can be determined by the equation Force (F) = mass (m) x acceleration (a)

(35.36) = 2 x a

Acceleration (a) = 35.36/3 = 17.68 m/sec²


Remarks:

The words magnitude and modulus mean the same thing with vectors In geometry magnitude and modulus mean the distance of the vector This is always a positive value The direction of the vector is irrelevant Magnitude or modulus is indicated by vertical lines |a| would mean the magnitude of vector a

Example: When the force of 50N inclined at 40 degress to the horizontal is resolved into its rectangular components the resulrs are as shown below:

Resolve the vector below into its rectangular components


Chapter 02

Get in touch, or swing by for a cup of coffee.

Chapter 03: Moments of Forces

Chapter 04: Frictional Forces

Chapter 05: Statics - Equilibrium of Rigid Bodies

Who we are and what we do.

Chapter 06: Vector Calculus

Chapter 07: Equations of Motion

Chapter 08: Newton's Laws of Motion

Chapter 09: Momentum and Collisions

Chapter 10

Who we are and what we do.

Chapter 11: Projectiles

Chapter 12: Inclined Planes

Incines planes - 1

Chapter 13: Tension Connected Particles

ASSUMPTIONS • Objects are modelled as masses concentrated at a single point so no rotational forces. • Strings are inextensible (inelastic) so any stretch can be disregarded • Strings and rods are light (no mass) so weight can be disregarded • Pulleys are smooth so no frictional force at the pully needs to be considered..

Chapter 14: Centroids and Center of Gravity

Chapter 15: Vector Differenital Equations

Chapter 16: Work Energy and Power

Chapter XX: Model Exam Paper