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DYNAMIC FORCES Equations of motion

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Page 1: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

DYNAMIC FORCESEquations of motion

Page 2: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

1, Acceleration (rate of change of Velocity)velocity is the vector version of speed, (speed in a straight line)

v – u t

= a u = initial velocity (in m/s)v= final velocity (in m/s)t = time (in seconds (s))a = m/s2

Can be rearranged

tov = u + at

Page 3: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question

•A car increases it’s velocity from 10 m/s to 20m/s in 5 seconds. What is it’s

acceleration?

Page 4: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question (answer)

v – u t

= a

20 – 10 5

= 2m/s2

v = 20m/s u =10m/s t = 5 sec

Page 5: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question

A car moving at 10 m/s accelerates at 2m/s2 for 4 seconds. What is it’s final

velocity?

Page 6: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question (answer)

v = u + at

v = 10 + 2 x 4 = 18m/s

Can be re-arranged to

u = 10m/s a = 2m/s2 t = 4 sec

Page 7: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question

•A stone block with a mass of 800Kg is lifted from rest with a

uniform acceleration by a crane such that it reached a velocity of

14m/s. after 10 seconds. Calculate the tension in the lifting

cable

Page 8: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question• To do this calculation we need to use another equation

• Force = mass x acceleration

• F = ma• Weight (force acting downwards) = mass x acceleration due to

gravity• Wt = mg

Wt = m x 9.81 (acceleration due to gravity on earth)

Page 9: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question (answer)

v – u = a v = a 14 = 1.4m/s2

t t 10

acceleration

Force due to acceleration

F = ma

Tension

Weight mg

U = 0 from standing start

First find the acceleration

Page 10: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question (answer)

F = ma F = 800 x 1.4 = 1120N Wt of box mg = 800 x 9.81 = 7848N (7.8kN)

Tension in cable = 1120 + 7848 = 8938N (8.9kN)

acceleration

Force due to acceleration

F = ma

Tension

Weight mg

Page 11: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question

• If the stone is lowered at the same rate of acceleration the tension is less than the weight

of the box

Tension in cable = 7848 - 1120 = 6728N (6.7kN)

Force due to acceleration

F = ma

Tension

acceleration

Weight mg

Page 12: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Lift

You get the same effect when you travel in a lift. You feel

heavier when the lift begins and accelerates upwards and lighter

when the lift accelerates downwards

Page 13: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

A man standing on weighing scales in a lift has a mass of 60 Kg. The lift accelerates uniformly at

a rate of 2m/s2 Calculate the reading on the scales during the period of acceleration .

Page 14: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

acceleration

Force due to acceleration

F = ma

Weight mg

Page 15: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

F = ma F = 60 x 2 = 120NWt of man mg = 60 x 9.81 = 588.6N Force acting on scale = 120 + 588.6 = 708.6N

The reading on the scale is 708.6 ÷ 9.81

= 72.23Kg

Page 16: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

2, Displacement (s) is the vector version of distance (distance in a straight line)

Displacement = average velocity x time

s = (v + u) x t 2

Page 17: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question

•A car moving at 10 m/s increases it’s velocity to 20m/s in 4 seconds. How far will it have travelled during

this time?

Page 18: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question (answer)

s = (v + u) x t 2

v =20m/s u = 10m/s t = 4 sec

s = (20 + 10) x 4 2

S = 60m

Page 19: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question

•How long will it take for an athlete to accelerate from rest to 4 m/s over 8m ?

Page 20: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample question (answer)

s = (v + u) x t 2

u =0 so s = v x t 2

t = 2s v

t = 16 = 4 seconds 4

Page 21: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

3, Displacement related to acceleration

s = ut + at2

2

With zero acceleration (constant velocity) a = 0 s = utFrom a standing start

ut = 0s = at2

2

Page 22: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

•A car accelerates uniformly from rest and after 12 seconds has

covered 40m. What are its acceleration and its final velocity ?

Page 23: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

2s = at2

2s = a t2

80 = a122

80 = a144

a = 0.56m/s2

Page 24: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Finding v

a = v – u t

From a standing start u = 0

a = v t

v = a x t

v = a x t v = 0.56 x 12 = 6.7 m/s

Page 25: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Or alternatively•

• U = 0 from standing start

s = (v + u) x t 2

s = v x t 2

v = 2s t

v = 80 = 6.7m/s 12

Page 26: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

4, final velocity, initial velocity acceleration and displacement

•v2 = u2 + 2 as

Page 27: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

If a car travelling at 10m/s accelerates at a constant rate of 2m/s2, what is it’s final velocity after it has travelled 10m?

Page 28: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Sample Question (answer)

v2 = u2 + 2 as

V2 = 102 + (2 x 2 x 10)

= 100 + 40 = 140m/s2

Page 29: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

D’Alembert’s Principle

Acceleration (a)

Applied Force (F)

Inertia Force (Fi)

F + Fi = 0 so F = -Fi

F = ma

so ma = - Fi

or Fi = - ma

When an object is accelerating the

applied force making it accelerate has to

overcome the inertia. This is the force which

resists the acceleration (or

deceleration) and is equal and opposite to the applied force. This

means that the total force acting on the

body is zero

mass

Page 30: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

D’Alembert’s Principle

Acceleration

Friction Force

20N

Applied Force

200N

Spring Force

150N

Mass

20Kg

Page 31: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Fr (Friction)

20N

W

(weight)

Mg =

20 x 9.81

=196.2N

F (applied)

200N

Fs (spring)

150N

Free body diagram

Page 32: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

D’Alembert’s Principle

•Downward forces are minus and upward forces are positive.

•From the diagram• -200N – 196.2N +20N +150N

•= -226.2N (which is downward as to be expected)

Page 33: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Conservation of energy (Gravitational potential energy)

10m

5Kg

GPE = mass x gravity x height

(mgh)=

5 x 9.81x10

490.5joules

Work done (in lifting the mass) = force

x distance49.05 x 10

= 490.5joules

(F = mg)

Work done = energy gained

Page 34: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Kinetic energy

10m

5Kg

GPE = mgh = 490.5 joules

KE (at the bottom) =490.5J =

mv2 2

(v = velocity)

Neglecting friction, all the GPE at the top of the slope converts to kinetic energy

at the bottom

Page 35: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Kinetic energy

10m

5Kg

GPE = mgh = 490.5 joules

The velocity at the bottom v =√(2Ke÷m)

= √ (2 x 490.5 ÷ 5)√196.2

= 14m/s

Neglecting friction, all the GPE at the top of the slope converts to kinetic energy

at the bottom

Page 36: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Work and energy

Force

distance

Work done (in joules) = Force x distance moved (in direction of force)

Work done = energy used

Page 37: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

•A car of mass 800Kg is stood on a uniform 1 in 10 slope when it’s handbrake is

suddenly released and it runs 30 metres to the bottom of the slope against a uniform frictional force of 50N. What is the car’s

velocity at the bottom of the slope?

Page 38: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

• First find the angle of the slope

1

10

Tan of the angle = opposite/adjacent =

1/10= 0.1Tan-1 0.1 = 5.7o

Page 39: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

• Then find the height of the slope • sin 5.7o = opposite/hypotenuse

• Opposite = hypotenuse x sine5.7o

• 30 x sine 5.7o

• =2.98mht

30m

5.7o

Page 40: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 1 (conservation of energy method)

• Find the gravitational potential energy of the car at the top of the slope

• 800 x 9.81 x 2.98• = 23.4kN

ht

30m

5.7o

Page 41: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 1 (conservation of energy method)

• Work done against friction = force x distance = 50N x 30m = 1.5kj

ht

30m

5.7o

Page 42: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 1 (conservation of energy method)

• Kinetic energy of the car at the bottom of the slope

mv2/2 = 23.4 -1.5 = 21.9kjv= √(2 x Ke/m)

v= √(2 x 21900/800) v= √54.75

v = 7.4 m/s •

ht

30m

5.7o

Page 43: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 2 (Resolving forces method)

• Work out the forces involvedWeight of car (force

acting vertically downward) = mass x

gravity= 800x 9.81

7848N

ht

30m

5.7o

Page 44: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 2 (Resolving forces method)

• Work out the forces involved

5.7o

5.7o

Fn

Fs

wt

Wt = weight of car (7848N)

Fn is the normal reaction force of the slope on the car

Fs is the force on the car down the slope

Page 45: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 2 (Resolving forces method)

• Work out the forces involved Sine 5.7o = Fs ÷ wt

Fs = Wt x sin 5.7o

Fs = 7848 sin 5.7o Fs = 779.5N (Force down the slope)

5.7o

5.7o

Fn

Fs

wt

Page 46: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 2 (Resolving forces method)

• Work out the forces involved

Resultant force down the slope = Fs – friction force

779.5 – 50 =749.5N

5.7o

5.7o

Fn

Fs

wt

Page 47: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 2 (Resolving forces method)

Acceleration down the slope a= F/m

749.5/800= 0.94m/s2

5.7o

5.7o

Fn

Fs

wt

Page 48: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example 2 (Resolving forces method)

Velocity at the bottom of the slope

v2 = u2 + 2as (u2 = 0) so

v2 = 2asv2 = 2 x 0.94 x 30

v =√56.4v = 7.5m/s

5.7o

5.7o

Fn

Fs

wt

Page 49: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Linear Momentum and Collisions• Conservation of Energy•

Page 50: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

•Momentum = mass x velocity

•The total momentum remains the same before and after a collision

•Momentum is a vector quantity

Page 51: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Linear Momentum and Collisions•A railway coach of mass 25t is moving along a

level track 36km/hr when it collides with and couples up to another coach of mass 20t

moving in the same direction at 6km/hr. Both of the coaches continue in the same direction

after coupling. What is the combined velocity of the two coaches?

Page 52: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Linear Momentum and Collisions

•Let the mass of the first coach be M1 and the mass of the second coach be M2 and the velocity of the first coach be V1 and the velocity of the second

be V2

Page 53: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Linear Momentum and Collisions

•Before coupling the momentum of the first coach is 25 x 36 = 900tkm/hr and the

momentum of the second is 20 x 6 =120 tkm/hr

•Which is a total of 1020tkm/hr

Page 54: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Linear Momentum and Collisions•After the coupling the momentum of both is the

same as before the coupling which is 1020 tkm/hr

•And the combined mass is 45t

Page 55: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Linear Momentum and Collisions•Velocity after coupling is momentum divided by

mass•1020÷45

•22.6 km/hr

Page 56: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

A hammer of mass 200Kg falls 5m on to a pile of mass 300Kg and drives it 100mm into the ground

a) Calculate the loss of energy on the impact.

b) Calculate the work done by the resistance of the ground.

c) calculate the average resistance to penetration.

Page 57: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example • Before falling the GPE of the hammer is 200kg x 9.81 x 5m = 9810j

• Kinetic energy of the hammer just before impact = 9810j (0.5 x m x v2)

• Velocity of the hammer just before impact v2 = (9810)/0.5 x m• (9810)/0.5 X 200 =98.1• v = √98.1 = 9.9m/s

Page 58: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

• Momentum of hammer just before impact = mass x velocity• = 200kg x 9.9m/s = 1980 kgm/s

• Momentum before collision = momentum after collision• mass of hammer plus pile after collision = 200kg + 300kg = 500kg

• thus 500kg x velocity after collision = 1980 kgm/s

• Velocity after collision = 1980 ÷ 500 = 3.96m/s

Page 59: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

•Kinetic energy after collision (0.5 x mass x v2) = 0.5 x 500 x 3.962

• = 3920j•Loss of energy = 9810 – 3920 = 5890j

• To find deceleration of pile hammer•v2 = u2 +2as (v2 =0)

•u2 = - 2as•

Page 60: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

•a = - u2/2s•3.962/0.2

• - 78.4m/s2

•The minus sign means deceleration, Resistive force of the ground = mass x deceleration

•500 x78.4•39.2kN

Page 61: DYNAMIC FORCES Equations of motion. 1, Acceleration (rate of change of Velocity) velocity is the vector version of speed, (speed in a straight line) v

Example

•Work done by ground = Force x distance •39.2kN x 0.1 m

•3.92kj

(this agrees with the fact that fact that the kinetic energy of the hammer and pile after impact was 3.92kj and zero when the pile

stopped moving in the ground