Sunday 29 May 2016

Term 2 Week 5 2016

Homework

Make sure that you have completed:


  • Ex 1, p.25-28, Translational Motion
  • Q2, Handout, Lab Exercise

New Homework

  • Ex 2, p. 41-45, Rotational Motion

Rotational Momentum (Angular Momentum)

For a point mass L = Pr

Linear Momentum times the radius distance between the point mass and the axis of rotation
Momentum: Rotational Linear
Equation: L = I P = mv
Units: kgm2s-1  kgms-1

  • Rotational Momentum and Linear Momentum have different units so they cannot be equated with each other and are independent of each other.
  • Rotational Momentum obeys the same law of conservation that Linear Momentum obeys. In the absence of outside forces, total momentum is always conserved.

Precession





Egg Spinning



Rotational Kinetic Energy

Energy: Rotational Linear
Equation: Ek(rot) = ½I2 Ek(lin) = ½mv2
Units: Joule Joule

  • Rotational Kinetic Energy and Linear Kinetic Energy have the same unit so they can be equated with each other and are interdependent on each other.
  • The law of conservation of total energy can be applied with all types of energy. You will be using mostly gravitational potential, linear kinetic, and rotational kinetic energies.

  • Total Kinetic Energy = Ek(rot) + Ek(lin)
= (½I⍵2) + (½mv2 )



Sunday 22 May 2016

Term 2 Week 4 2016

Homework

Make sure that you have completed:


  • Ex 1, p.25-28, Translational Motion
  • Q2, Handout, Lab Exercise

Rotational Motion:

  • Q1, p.31 Rotational Kinematics

Rotational Kinematics


Radian Measure

Radian Measure is used so that we can easily calculate an arc length, d (m), given an angle, š›‰ (Rad) and the radius, r (m).

d = rš›‰

This in turn allows us to relate velocity, v (ms-1) to angular velocity ⍵ (rads-1), in the same way.

v = r⍵

also ⍵ = 2š…f

 This also allows us to relate acceleration, a (ms-2), to angular acceleration, Ī± (rads-2), in the same way.

a = rĪ±

The rotational kinematics work just like the translational kinematic equations when there is a constant acceleration.

  • f = ⍵i + Ī±t vf = vi + at
  • f2 = ⍵i2 + 2Ī±š›‰ vf2 = vi2 + 2ad
  •  š›‰ = ⍵it + ½Ī±t2 d = vit + ½a2
  •  š›‰ = ½(⍵i + ⍵f)t d = ½(vi + vf)t
Rotational Inertia



Torque

Wednesday 18 May 2016

Term 2 Week 3 2016

Physics 3.1 AS 91521 Lab Investigation


How to use Excel for the lab investigation

Mass on a Spring Part 1 - finding average & period

Mass on a Spring Part 2 - Gathering the Raw Data


Mass on a Spring Part 3 - Transforming the Raw Data

Mass on a Spring Part 3a - Correction on Transforming the Raw Data

Mass on a Spring Part 4 - Applying Uncertainties to your Data

Mass on a Spring Part 5 - Transforming Uncertainties

Mass on a Spring Part 6 - Adding Error Bars to your Graph

Mass on a Spring Part 7 - Line of Worst Fit

Sunday 15 May 2016

Term 2 Week 2 2016

Homework


  • Handout Q2, Lab
  • Ex 1, p, 25-28 Linear Motion

2D Momentum

Part 1

Part 2

Circular Motion

  • Vertical Circle





  • Banked Corners


  • Orbital Motion


Satellite Motion


Term 2 Week 1 2016

Homework:

  • Handout Q2 Lab
  • Ex 1, P.21-28 Linear Motion

Translational Motion


Linear Motion

  • Newton’s Laws of Motion




Newton's Third Law


  • Free Body Diagrams


Tension Free Body Diagram


  • Center of Mass

Wednesday 4 May 2016

Term 1 Week 11 2016

Assessment Week for Phy 3.7 Socio-Scientific Issue


Then Introduction of Errors for Phy 3.1 Lab Investigation


  • Analog Scale: error is half the smallest scale division
  • Digital Reading: error is the one of the last digits on the reading
  • Adding or Subtracting: Add the actual errors
  • Multiplying or Dividing: Add the percentage errors
  • Power: Multiply the percentage error by the power