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2014 SEPT - MECHANICS REG REVIEW.pdf

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Page 1: 2014 SEPT - MECHANICS REG REVIEW.pdf
Page 2: 2014 SEPT - MECHANICS REG REVIEW.pdf

Rowel Allan Rocaberte, REE, ECE

Page 3: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Beam

- A slender bar that carries transverse loading, that is, the applied forces are perpendicular to the bar

- Horizontal structural element that is capable of withstanding load primarily by resisting bending

Cantilever Beam

- Anchored at only one end

Overhanging Beam

- Asymmetrical placing of supports

In a beam, the internal force system consists of a shear force and a bending

moment acting on the cross section of the bar.

The internal forces give rise to two kinds of stresses on a transverse section of a beam: (1) axial stress that is caused by the bending moment and (2) shear stress due to the shear force.

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

No need to discuss derivation. Dati naman hindi na.

Page 4: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Beams are classified according to their supports.

Fixed Beam

Simply Supported Beam

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

. .

P

P

No need to discuss derivation. Dati naman hindi na.

Page 5: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Beams are classified according to their supports.

Cantilever Beam

Overhanging Beam

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

. .

ω

R M

ω P

R1 R2

No need to discuss derivation. Dati naman hindi na.

Page 6: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Loading Principles:

Uniformly Distributed Load Effective Resultant &

Moment Arm

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

ω

L

R = ωL

L/2

No need to discuss derivation. Dati naman hindi na.

Page 7: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Loading Principles:

Uniformly Varying Load Effective Resultant &

Moment Arm

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

ω

L

R = ½ ωL

2/3 L

No need to discuss derivation. Dati naman hindi na.

Page 8: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Loading Principles:

Combination of Distributed Effective Resultant &

and Uniformly Varying Loads Moment Arm

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

ω2

L

R2 = ½ (ω2-ω1)L

2/3 L

ω1

ω2 - ω1

L/2

R1 = ω1L

No need to discuss derivation. Dati naman hindi na.

Page 9: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Shear and Moment Diagrams

- Analytical tools used in conjunction with structural analysis to help perform structural design by determining the value of shear force and bending moment at a given point of an element

- Convenient visual references to the internal forces in a beam, in particular, they identify the maximum values of τ and M.

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

Read also the slides on Beams by M. S. Sivakumar from Indian Institute of Technology Madras as

supplement

No need to discuss derivation. Dati naman hindi na.

Page 10: 2014 SEPT - MECHANICS REG REVIEW.pdf

R

Shear and Moment Diagrams

Sign conventions

R. Rocaberte || MECH 313 © 1st Sem 2013-2014

External Loads

Shear Force

Bending Moment

Positive Negative

ω P M

ω P

M

V

V

V

V

M M M M

No need to discuss derivation. Dati naman hindi na.

Page 11: 2014 SEPT - MECHANICS REG REVIEW.pdf

55. Which of the following support or connection has two unknowns?

A. Roller Support C. Short Link

B. Rocker Support D. Hinge Support

Page 12: 2014 SEPT - MECHANICS REG REVIEW.pdf

56. A simple beam, 10 m long carries a concentrated load of 500 kN at the midspan. What is the maximum moment of the beam in kN-m?

A. 250

B. 500

C. 1000

D. 1250

Page 13: 2014 SEPT - MECHANICS REG REVIEW.pdf

57. Determine the maximum moment of the beam loaded as shown in kN-m.

A. 125

B. 175

C. 875

D. 1250

5m 10m

200 kN

R1

R2

5m

100 kN

Page 14: 2014 SEPT - MECHANICS REG REVIEW.pdf

58. It occurs when a member carries a load perpendicular to its long axis while being supported in a stable manner.

A. Direct shear C. Torsional shear

B. Bending stress D. Torsional stress

Bending Stress a.k.a Moment Stress

Page 15: 2014 SEPT - MECHANICS REG REVIEW.pdf
Page 16: 2014 SEPT - MECHANICS REG REVIEW.pdf

RADIUS OF GYRATION

59. What is the radius of gyration of a 5-inch square with respect to its centroidal axis?

A. 1.44 in C. 10.39 in

B. 0.866 in D. 0.5 in square

ak =

12

4

2

square

aI 12k = =A a

5k = = 1.44 in

12

Page 17: 2014 SEPT - MECHANICS REG REVIEW.pdf

SECTION MODULUS

60. What is the section modulus of a 5-inch square with respect to its centroidal axis?

A. 20.83 cm3 C. 25.7 cm3

B. 49.5 cm3 D. 57.2 cm3

4

squaresquare

3

square

33

square

Ise mo =

y

aI 12z = =ay

2

az =

6

5z = = 20.83 in

6

Page 18: 2014 SEPT - MECHANICS REG REVIEW.pdf

61. What is the formula of the radius of gyration, k, of a circular cross-section with diameter D?

A. B.

C. D.

1k D

18

1k D

12

1k D

4

1k D

12

Page 19: 2014 SEPT - MECHANICS REG REVIEW.pdf

62. What is the formula of the section modulus, z, of a rectangle?

A. B.

C. D.

3bhZ

6

2bhZ

36

3bhZ

36

2bhZ

6

Page 20: 2014 SEPT - MECHANICS REG REVIEW.pdf

63. What is the moment of inertia of a cylinder of radius 5 m and mass of 5 kg?

A. 62.5 kg-m2 B. 80 kg-m2

C. 72.5 kg-m2 D. 120 kg-m2

Page 21: 2014 SEPT - MECHANICS REG REVIEW.pdf

- oldest branch of Physics.

- study of the bodies and systems and the forces acting on them.

Page 22: 2014 SEPT - MECHANICS REG REVIEW.pdf
Page 23: 2014 SEPT - MECHANICS REG REVIEW.pdf

1. Which of the following refers to the branch of mechanics dealing with the motion of bodies?

A. Kinematics

B. Kinetics

C. Dynamics

D. Statics

Page 24: 2014 SEPT - MECHANICS REG REVIEW.pdf

Force

• The scientific definition for force is simply a push or a pull. For example, when you do homework you exert a force on your pen or pencil because you push and pull it across the paper.

Page 25: 2014 SEPT - MECHANICS REG REVIEW.pdf

Net Force

• The sum of the forces is called the net force. In this case the net force is an unbalanced force. An unbalanced force is a force that changes an object’s motion or causes it to accelerate. The arrows show different forces and their direction, the wider the arrow the stronger the force.

Page 26: 2014 SEPT - MECHANICS REG REVIEW.pdf
Page 27: 2014 SEPT - MECHANICS REG REVIEW.pdf
Page 28: 2014 SEPT - MECHANICS REG REVIEW.pdf

Force and Force Systems

• Collinear Forces are forces that act on the same line of action

• Parallel Forces are forces that are of the same angle to one another. Couple is a pair of parallel forces of the same magnitude but opposite in direction.

• Frictional Force is a force that always acts in opposite direction to the applied force.

Page 29: 2014 SEPT - MECHANICS REG REVIEW.pdf

Force and Force Systems

• Coplanar Forces are forces lying on the same plane.

• Concurrent Forces are forces that meet in one common point.

• Non-concurrent Forces are forces that do not meet in one common point.

Page 30: 2014 SEPT - MECHANICS REG REVIEW.pdf

A quantity that has magnitude (and unit) only.

E.g. speed, distance, volume, current & etc.

A quantity that has magnitude, (unit) and direction. E.g. force gravity, displacement, acceleration, momentum, etc.

Page 31: 2014 SEPT - MECHANICS REG REVIEW.pdf

SCALARS VECTORS

Mass A load has a mass of 5kg.

Weight / Force A force of 15 N acts on a body in an upward direction.

Distance The train has traveled a distance of 80 km.

Displacement An airplane flies a distance of 100km in an easternly direction.

Speed Velocity A car moves 60km/hr, 35⁰ east of north.

Time The car has reached its destination after 1 hr.

Acceleration

Page 32: 2014 SEPT - MECHANICS REG REVIEW.pdf

Addition: A + B = B + A Subtraction: A – B Multiplication: Dot Product: A · B Cross Product: A x B

Page 33: 2014 SEPT - MECHANICS REG REVIEW.pdf

The sum of two or more vectors is represented by a single vector called resultant.

This resultant vector may be found by using:

– Graphical Method

– Pythagorean Theorem

– Component method

Page 34: 2014 SEPT - MECHANICS REG REVIEW.pdf

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

MECH 312 RROCABERTE © 2013

Page 35: 2014 SEPT - MECHANICS REG REVIEW.pdf

CABLES

Used in numerous engineering applications (suspension bridges, power transmission lines, cable supporting heavy trolleys or telephone lines)

Incapable of developing internal forces other than TENSION

TWO TYPES:

1. Parabolic

2. Catenary

Front slide photo taken from http://catenary-project.wikispaces.com/Golden+Gate+Bridge

MECH 312 RROCABERTE © 2013

Page 36: 2014 SEPT - MECHANICS REG REVIEW.pdf

PARABOLIC CABLES: Symmetric

- Loading is distributed uniformly along the horizontal

L = span; distance between supports (m, ft)

d = sag ; maximum vertical displacement (m, ft)

S = total length of the cable (m, ft) Photo taken from http://www.solutioninn.com/engineering/civil-engineering/statics/the-cable-is-subjected-to-the-parabolic-loading-w-w0-18722-2xa

L

d S

5

6

3

42

7

256

5

32

3

8

L

d

L

d

L

dLS

ω

MECH 312 RROCABERTE © 2013

Page 37: 2014 SEPT - MECHANICS REG REVIEW.pdf

PARABOLIC CABLES: Symmetric

ω = load per horizontal length (N/m, lb/ft)

T = tension at the supports (N, lb)

H = tension at the lowest point (N, lb)

S/2

T

H

Photo taken from http://www.solutioninn.com/engineering/civil-engineering/statics/the-cable-is-subjected-to-the-parabolic-loading-w-w0-18722-2xa

L/2

2

2

2

1

LωHT

ω

2

FBD:

T

H

2

MECH 312 RROCABERTE © 2013

Page 38: 2014 SEPT - MECHANICS REG REVIEW.pdf

PARABOLIC CABLES: Symmetric

Photo taken from http://www.solutioninn.com/engineering/civil-engineering/statics/the-cable-is-subjected-to-the-parabolic-loading-w-w0-18722-2xa

d

LωH

8

2

042

)(0

dHLLω

cwM AT

H

L/2

2

d

MECH 312 RROCABERTE © 2013

S/2

Page 39: 2014 SEPT - MECHANICS REG REVIEW.pdf

PARABOLIC CABLES: Unsymmetric

- x and y axes are placed on the lowest point

- analyzed like two separate symmetric cables

Photo taken from http://www.mathalino.com/forum/strength-materials/parabolic-cable

O

L

dA

dB

2

LA2

LB

MECH 312 RROCABERTE © 2013

Page 40: 2014 SEPT - MECHANICS REG REVIEW.pdf

2. A pipeline crossing a river is suspended from a steel cable stretched between two posts 100 m apart. The weight of the pipe is 14 kg/m while the cable weighs 1 kg/m assumed to be uniformly distributed horizontally. If the allowed sag is 2 m, determine the tension of the cable at the post.

A. 9047.28 kg B. 9404.95 kg

C. 9545.88 kg D. 9245.37 kg

L = 100m; w = 15kg/m; d = 2m H = wL2/8d H = (15)(100)2 / 8(2) = 9375 kg T2 = H2 + [(1/2)wL]2

T = sqrt [93752 + (1/2 x 15 x 100)2 ] = 9404.95 kg

Page 41: 2014 SEPT - MECHANICS REG REVIEW.pdf

3. A certain cable is suspended between two supports at the same elevation and 500 ft apart. The load is 500 lbs per horizontal foot including the weight of the cable. The sag of the cable is 30 ft. Calculate the total length of the cable.

A. 503.21 ft B. 504.76 ft

C. 505.12 ft D. 506.03 ft

Page 42: 2014 SEPT - MECHANICS REG REVIEW.pdf

The Catenary Curve MECH 312 RROCABERTE © 2013

Gateway Arch in St. Louis, Missouri [1]

Spider’s web [2]

Hanging chain [3]

Lace [5]

Freely-hanging transmission lines [4]

a

xay cosh

Dance Step Exercise:

Hawi – Sine (wave) – Wax ng Hair)

Galileo claimed that the curve of a chain hanging under gravity should be a parabola. In 1669, his claim was proved to be wrong.

Page 43: 2014 SEPT - MECHANICS REG REVIEW.pdf

Galileo

• called the father of modern science precisely because he initiated the comparison between theory and experiment

Page 44: 2014 SEPT - MECHANICS REG REVIEW.pdf

“Big Bang is the Day without Yesterday” - Msgr. George Lemaitre

• Lemaitre told Einstein, “Your mathematics is correct, but your physics is abominable!”

Page 45: 2014 SEPT - MECHANICS REG REVIEW.pdf

- Loading is distributed uniformly along the length of the cable

L = span (m, ft)

y = sag(m, ft)

S = total length of the cable (m, ft)

CATENARY CABLES: Symmetric

Photo taken from http://lecture.civilengineeringx.com/structural-analysis/structural-steel/suspension-bridge-analysis/

L

y

S

T T

ω

MECH 312 RROCABERTE © 2013

A B

Page 46: 2014 SEPT - MECHANICS REG REVIEW.pdf

SAO = length of the cable from A to O (m, ft)

x = horizontal span from A to O (m, ft)

H = tension at the lowest point (N, lb)

ω = weight per unit length of the cable (N/m, lb/ft)

CATENARY CABLES: Symmetric

Photo taken from http://lecture.civilengineeringx.com/structural-analysis/structural-steel/suspension-bridge-analysis/

y SAO

T

ω

MECH 312 RROCABERTE © 2013

A

x

H O

H

ω

HSAO sinh

1cosh

H

ω

Hy

Page 47: 2014 SEPT - MECHANICS REG REVIEW.pdf

T = tension at the supports (N, lb)

Recall equation of a catenary

CATENARY CABLES: Symmetric

Photo taken from http://lecture.civilengineeringx.com/structural-analysis/structural-steel/suspension-bridge-analysis/

T

MECH 312 RROCABERTE © 2013

x

H

22

AOSωHT

AOSω

FBD:

T

H

AOSω

yωHT

a

xay cosh H

xωHT cosh

y

Page 48: 2014 SEPT - MECHANICS REG REVIEW.pdf

Note:

For symmetric catenary cables,

If , you may solve catenary cable problem as

a parabolic cable.

(A small sag-to-span ratio means that the cable is tight, and the uniform distribution of weight along the cable is not very different from the same load intensity distributed uniformly along the horizontal.)

CATENARY CABLES: Symmetric MECH 312 RROCABERTE © 2013

Ly10

1

AOSS

xL

2

2

Page 49: 2014 SEPT - MECHANICS REG REVIEW.pdf

Similar to parabolic (unsymmetric):

- x and y axes are placed on the lowest point

- analyzed like two separate symmetric cables

CATENARY CABLES: Unsymmetric

Photo taken from http://lecture.civilengineeringx.com/structural-analysis/structural-steel/suspension-bridge-analysis/

L

TB

TA

MECH 312 RROCABERTE © 2013

A

B

x

y

O SAO

SOB

Page 50: 2014 SEPT - MECHANICS REG REVIEW.pdf

4. A cable which has a mass of 0.6 kg/m and is 240 m long is to be suspended with a sag of 24 m. Determine the tension at midlength, maximum tension and maximum span.

A. 233.55 m

B. 240 m

C. 265.216 m

D. 190.98 m

MECH 312 RROCABERTE © 2013

22

AOSωHT

yωHT

H = 1696.39 T = 1837.75

H

xωHT cosh

x = 116.78 L = 2x = 233.55 m

Page 51: 2014 SEPT - MECHANICS REG REVIEW.pdf
Page 52: 2014 SEPT - MECHANICS REG REVIEW.pdf

MECH 312 UNIT 1

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

Page 53: 2014 SEPT - MECHANICS REG REVIEW.pdf

Speed

The average speed of an object is equal to the total distance traveled in a given unit of time. It is a scalar quantity because it has no direction .

t

dvs

Speed and velocity are often used interchangeably in ordinary conversations. In physics, there is a clear distinction between these two concepts.

Page 54: 2014 SEPT - MECHANICS REG REVIEW.pdf

Velocity We define velocity as the time rate of change of

position.

The velocity of an object moving along a straight path is equal to the slope of the d-against-t graph. When the graph is a straight line, the velocity is constant.

Page 55: 2014 SEPT - MECHANICS REG REVIEW.pdf

Velocity The average velocity of an object is the total

displacement divided by the elapsed time.

t

dvave

Page 56: 2014 SEPT - MECHANICS REG REVIEW.pdf

Velocity

Instantaneous velocity is the velocity of the object at a particular instant. Its magnitude is equal to the slope of the line tangent to the point corresponding to the given time t.

iedt

dsv ˆ

vectorgentunitei tanˆ

Page 57: 2014 SEPT - MECHANICS REG REVIEW.pdf

Acceleration We define acceleration as the time rate of

change of velocity.

average instantaneous

acceleration acceleration

t

vaave

dt

vda

Page 58: 2014 SEPT - MECHANICS REG REVIEW.pdf

Rectilinear Translation Rectilinear Translation

A type of motion in which a body moves in a straight line or is moving in the direction parallel to its displacement.

Uniform Motion

A motion with constant speed or velocity [a = 0]

Uniformly Accelerated Motion

A motion with constant change in velocity or of uniform acceleration [a is (+) is accelerating or speeding up; a is (-) if decelerating or slowing down]

D1.

Page 59: 2014 SEPT - MECHANICS REG REVIEW.pdf

Kinematic Differential Equations of Motion

s = displacement

v = velocity

a = acceleration

t = time

dt

dsv )1(

dt

dva )2(

dvvdsa )3(a

dv

v

ds

andfrom

),2()1(

Page 60: 2014 SEPT - MECHANICS REG REVIEW.pdf

Rectilinear Translation For uniformly accelerated motion along a

straight horizontal path:

atvv

asvv

attvs

o

o

o

2

2

1

22

2

s = displacement vo = initial velocity v = final velocity a = acceleration t = elapsed time Uniform velocity: a = 0, v = vo

Starting from rest: vo = 0 Stop at a point: v = 0

Page 61: 2014 SEPT - MECHANICS REG REVIEW.pdf

5. From the speed of 100 kph, a car decelerates at the rate of 15 m/min/sec along a straight road. Which of the following gives the distance travelled at the end of 40 sec.

A. 3800 m

B. 911.112 m

C. 91.111 m

D. 455.56 m

V0 = 100kph x 1000

/3600 = 27.7778 m/s

a = -15/60 mps2 = -0.25

mps2

s = 27.7778(40) + 0.5(-

0.25)(40)2 = 911.112 m

Page 62: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: An airplane lands on a carrier deck at 200 mi/h and is brought to a stop uniformly, by an arresting device, in 50 ft. Find the time required to stop.

• A. 0.34 sec C. 0.46 sec

• B. 0.21 sec D. 0.86 sec

There’s no other way but up!

0.34 sec

Page 63: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: A sports car starting from rest can attain a speed of 60 mi/hr in 8 seconds. A runner can do a 100-yard dash in 9.8 seconds. Assume that the runner is moving with uniform speed and that the car starts at the instant he passes it. How far will both travel until the car overtakes the runner?

• A. 180.3 ft C. 200.3 ft

• B. 190.3 ft D. 170.3 ft

There’s no other way but up!

170.3 ft

Page 64: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: What average net thrust must a 17-ton airplane have in order to reach an altitude of 5,000 ft and a speed of 600 mi/hr at an airline distance of 10 mi from its starting point?

• A. 11,000 lb C. 14,000 lb

• B. 13,000 lb D. 12,000 lb

There’s no other way but up!

11,000 lb

Page 65: 2014 SEPT - MECHANICS REG REVIEW.pdf

6. An airplane acquires a take-off velocity of 150 mph on a 2-mile runway. If the plane started from rest and the acceleration remains constant, what is the time required to reach take-off speed?

A. 40 s B. 45 s

C. 58 s D. 96 s

Page 66: 2014 SEPT - MECHANICS REG REVIEW.pdf

MECH 312 UNIT 1

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

Page 67: 2014 SEPT - MECHANICS REG REVIEW.pdf

Free Falling Body - straight line free fall

- motion in vertical direction

ga

For free fall: where g = acceleration due to gravity = 9.81 m/s2 = 32.2 ft/s2

Page 68: 2014 SEPT - MECHANICS REG REVIEW.pdf

Free Falling Body Same formulas for rectilinear motion

gtvv

gyvv

gttvy

o

o

o

2

2

1

22

2

Page 69: 2014 SEPT - MECHANICS REG REVIEW.pdf

Free Falling Body

from A to B: y (+) v (+) g (-) from B to C: y (+) v (-) g (-) from C to D: y (-) v (-) g (-)

B (highest point)

A C (reference point)

D

Page 70: 2014 SEPT - MECHANICS REG REVIEW.pdf

Free Falling Body

y (+) above the reference point

y (-) below the reference point

v (+) upward motion

v (-) downward motion

g (-) always negative

B (highest point)

A

D

C (reference point)

Page 71: 2014 SEPT - MECHANICS REG REVIEW.pdf

7. A stone is thrown down from the top of the cliff 150 m high with an initial speed of 30 m/sec. How long will it take to reach the bottom?

A. 3 sec B. 2.5 sec

C. 4.56 sec D. 3.26 sec

Page 72: 2014 SEPT - MECHANICS REG REVIEW.pdf

8. A ball is thrown vertically upward from the ground and a student gazing out of a window sees it moving upward pass him at 5 m/s. The window is 10 m above the ground. How high does the ball go above the ground?

A. 1.276 m

B. 11. 276 m

C. 5.276 m

D. 15.276 m

MECH 312 RROCABERTE © 2013

10

222

hH

ghvv o

Page 73: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: A stone is dropped down a well and 5 seconds later the sound of the splash is heard. If the velocity of sound is 1120 ft/s, what is the depth of the well? Ans. 353.31 ft

MECH 312 RROCABERTE © 2013

Page 74: 2014 SEPT - MECHANICS REG REVIEW.pdf

MECH 312 UNIT 1

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

Page 75: 2014 SEPT - MECHANICS REG REVIEW.pdf

Projectile Motions

• A projectile is an object or body thrown with an initial velocity and whose motion is influenced by the pull of gravity

Page 76: 2014 SEPT - MECHANICS REG REVIEW.pdf

Projectile Motions

• Projectile motion is the motion of a body (the projectile) with a constant acceleration.

• It is principally determined by two types of motion: vertical and horizontal motions.

• Trajectory is the path of a projectile. Projectiles follow a parabolic path.

Page 77: 2014 SEPT - MECHANICS REG REVIEW.pdf

222

2

cos2

cos

cos2

1

θvxavv

θvtavv

tθvattvx

oxoxx

oxoxx

oox

Flight of Projectile

θ

xmax

vo

voy

vox

y = 0 y = 0

vy = 0

ymax

gyθvyavv

gtθvtavv

gttθvtatvy

oyoyy

oyoyy

oyoy

2sin2

sin

2

1sin

2

1

222

22

θvv

θvv

ga

a

motionprojectileFor

ooy

oox

y

x

sin

cos

0

,

Page 78: 2014 SEPT - MECHANICS REG REVIEW.pdf

Range of a Projectile

g

θvR

g

θθv

g

θvθv

tθvtvxR

g

θvt

gttθv

yRangeforgttvy

o

ooo

oox

o

o

o

2sin

cossin2sin2cos

cos

sin2

2

1sin0

0,;2

1

2

2

max

2

2

Page 79: 2014 SEPT - MECHANICS REG REVIEW.pdf

Height of a Projectile

g

θvH

gHθv

vHeighttheat

gHvv

o

o

fy

oyfy

2

sin

2sin0

0,max

2

22

22

22

Page 80: 2014 SEPT - MECHANICS REG REVIEW.pdf

If final position is not the same as the original level, we have values for both x and y

θv

gxθxy

θv

gx

θ

θxy

θv

xg

θv

xθvy

θv

xtlet

gttθvy

tθvx

o

o

oo

o

o

o

o

22

2

22

2

2

2

cos2tan

cos2

1

cos

sin

cos2

1

cossin

cos

2

1sin

cos

Page 81: 2014 SEPT - MECHANICS REG REVIEW.pdf

Guide Question

9. A shot is fired at an angle of 45˚ with the horizontal and a velocity of 300 fps. Calculate the range of the projectile.

A. 3500 yd

B. 2800 yd

C. 1471 yd

D. 932 yd

Page 82: 2014 SEPT - MECHANICS REG REVIEW.pdf

Guide Question

10. A projectile leaves at a velocity of 50 m/s at an angle of 30˚ with the horizontal. Find the maximum height that it could reach in meter.

A. 41.26

B. 28.46

C. 31.86

D. 51.26

Page 83: 2014 SEPT - MECHANICS REG REVIEW.pdf

11. A projectile is fired from a cliff 300 m high with an initial velocity of 400 m/s. If the firing angle is 30° from the horizontal, compute the horizontal range of the projectile.

A. 15.74 km B. 14.54 km

C. 12.31 km D. 20.43 km

y=xtanθ-gx2/2(vocosθ)2

-300=(tan30)x-9.81/2(400cos30)2 x2

x=14.63km

Page 84: 2014 SEPT - MECHANICS REG REVIEW.pdf
Page 85: 2014 SEPT - MECHANICS REG REVIEW.pdf

at = r α

at = r ω2

Page 86: 2014 SEPT - MECHANICS REG REVIEW.pdf

12. The normal acceleration of a particle on the rim of a pulley 10 ft in diameter is constant at 1200 fps2. Which of the following gives the speed of the pulley in rpm.

a. 77.4597 b. 15.4919

c. 147.9371 d. 73.9686

an = v2/r, 1200 = v2/5,

v = 77.4597 fps

v = rω, 77.4597 = 5ω, ω

= 15.4919

rad/sec*60/2Π =

147.9371 rpm

Page 87: 2014 SEPT - MECHANICS REG REVIEW.pdf

13. A discus thrower moves the discus in a circle of radius 80.0 cm. At a certain instant, the thrower is spinning at an angular speed of 10.0 rad/s and the angular speed is increasing at 50.0 rad/s2. At this instant, find the tangential and centripetal components of the acceleration of the discus and the magnitude of the acceleration. a. 89.1 m/s2 b. 89.2 m/s2 c. 89.3 m/s2 d. 89.4 m/s2

2 2

tan

2 2 2

2 2 2

tan

(0.800 )(50.0 / ) 40.0 /

(10.0 / ) (0.800 ) 80.0 /

89.4 /

rad

rad

a r m rad s m s

a r rad s m m s

a a a m s

Page 88: 2014 SEPT - MECHANICS REG REVIEW.pdf

MECH 312 UNIT 2

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

Page 89: 2014 SEPT - MECHANICS REG REVIEW.pdf

Newton’s Laws of Motion

- The basis for extending the kinetics of a particle to a body composed of a system of particles.

“particle” – denotes an object of point size

“body” – denotes a system of particles which form an object of appreciable size

Any rigid body, regardless of its size, may be considered to be a particle if all of its parts move in identical parallel paths.

MECH 312 RROCABERTE © 2013

Page 90: 2014 SEPT - MECHANICS REG REVIEW.pdf

Newton’s Laws of Motion

First Law (Law of Inertia)

A body acted on by no net force moves with constant velocity (which may be zero) and zero acceleration.

Second Law (Law of Acceleration)

If a net external force acts on a body, the body accelerates. The direction of acceleration is the same as the direction of the net force.

Third Law (Law of Interaction)

If body A exerts a force on body B, then body B exerts a force on body A. These two forces are equal in magnitude but are opposite in direction; a.k.a. “Law of Action and Reaction”

MECH 312 RROCABERTE © 2013

aFFne t m

Page 91: 2014 SEPT - MECHANICS REG REVIEW.pdf

Newton’s Laws of Motion for a Particle

Inertia is the resistance a body offers to a change in its motion.

The reference frame or set of axes in which Newton’s laws are valid is one having a fixed origin and fixed directions of the axes. It is called an inertial, Newtonian, Galilean frame of reference.

Absolute motion - motion with respect to an inertial frame.

MECH 312 RROCABERTE © 2013

Page 92: 2014 SEPT - MECHANICS REG REVIEW.pdf

Every particle in the universe attracts every other particle with a force which is directly

proportional to the product of the masses of two particles and inversely proportional to the square of the distance between the centers of

the masses.

Newton’s Law of Universal Gravitation

Page 93: 2014 SEPT - MECHANICS REG REVIEW.pdf

Fg = gravitational force

G = 6.673 x 10-11 m3/kg-s2 (CONST 39)*

m1 & m2 = masses of the particles (kg)

r = center-to-center distance (m)

1 2

2g

m mF G

r

Gravitational Force

*Do not confuse G with acceleration g due to gravity.

Page 94: 2014 SEPT - MECHANICS REG REVIEW.pdf

Effective Force on a Particle

The effective force on a particle is defined as the resultant force on a particle, e.g. R or ma.

Inertia force the reaction caused by a resultant force

force numerically equal to ma but directed oppositely to the acceleration

Dynamic equilibrium: when inertia force is considered to act on a particle together with the resultant force, the particle is in a state of equilibrium.

MECH 312 RROCABERTE © 2013

Page 95: 2014 SEPT - MECHANICS REG REVIEW.pdf

D’Alembert’s Principle

The resultant of the external forces applied to a body (rigid or nonrigid) composed of a system of particles is equal to the vector summation of the of the effective forces acting on all particles.

The impressed forces acting on any body are in dynamic equilibrium with the inertia forces of the particles of the body.

MECH 312 RROCABERTE © 2013

P2

P1

W

332211

21

amamamR

PPWR

Page 96: 2014 SEPT - MECHANICS REG REVIEW.pdf

Newton’s Laws of Motion for a Particle

Newton’s second Law for any particle may now be expressed as

If the effective forces miai are reversed and considered to act on each respective particle of the system that the system will be in a state of balance known as dynamic equilibrium.

MECH 312 RROCABERTE © 2013

n

i

ii

n

i

i m11

aF

Page 97: 2014 SEPT - MECHANICS REG REVIEW.pdf

Guide Question

14. Riders in a bus are pushed forward during a sudden stop. Which law of motion provides an explanation?

A. Law of Inertia

B. Law of Interaction

C. Law of Universal Gravitation

D. Hooke’s Law

Page 98: 2014 SEPT - MECHANICS REG REVIEW.pdf

Guide Question

15. The force required to maintain an object at a constant speed in free space is equal to ____.

A. The weight of the object

B. The mass of the object

C. Zero

D. The force required to stop it

Page 99: 2014 SEPT - MECHANICS REG REVIEW.pdf

Guide Question

16. A rock is dropped out of the window of a moving car. At the same time a ball is dropped from the rest of the same height. Neglecting air resistance, which will reach the ground first?

A. Rock will hit the ground first.

B. Ball will hit the ground first.

C. Both will hit at the same time.

D. Neither will hit the ground.

Page 100: 2014 SEPT - MECHANICS REG REVIEW.pdf

MECH 312 UNIT 3

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

Page 101: 2014 SEPT - MECHANICS REG REVIEW.pdf

Translation: Analysis as a Particle

The fundamental equation of kinetics for a particle

MECH 312 RROCABERTE © 2013

aaR

FR

g

Wm

0

:

yy

xx

aF

aF

g

W

g

W

motionrrectilineaFor

tt

nn

aF

aF

g

W

r

v

g

W

g

W

motionrcurvilineaFor

2

:

Page 102: 2014 SEPT - MECHANICS REG REVIEW.pdf

17. Two blocks A and B are released from rest on a 30ᴼ incline when they are 60 ft apart. The coefficient of friction under the upper block A is 0.20 and that under the lower block B is 0.40. Compute the acceleration of block A as it moves down the incline. A. 11.52 m/s2 B. 12.52 m/s2m C. 14.52 m/s2 D. 10.52 m/s2

MECH 312 RROCABERTE © 2013

μA = 0.2

μB = 0.4 30o

Page 103: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: Two blocks A and B are released from rest on a 30ᴼ incline when they are 60 ft apart. The coefficient of friction under the upper block A is 0.20 and that under the lower block B is 0.40. Compute the acceleration of block B as it moves down the incline. Ans. 4.946 m/s2

MECH 312 RROCABERTE © 2013

μA = 0.2

μB = 0.4 30o

Page 104: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: Two blocks A and B are released from rest on a 30ᴼ incline when they are 60 ft apart. The coefficient of friction under the upper block A is 0.20 and that under the lower block B is 0.40. Compute the elapsed time until the blocks touch. Ans. 4.56 sec

MECH 312 RROCABERTE © 2013

μA = 0.2

μB = 0.4 30o

Page 105: 2014 SEPT - MECHANICS REG REVIEW.pdf

Centripetal Force

A force that makes a body follow a curved path: it is always directed orthogonal to the velocity of the body.

A force which keeps a body moving with a uniform speed along a circular path and is directed along the radius towards the center.

from Latin centrum meaning "center" and petere, meaning "to seek"

Page 106: 2014 SEPT - MECHANICS REG REVIEW.pdf

Centrifugal Force

Represents the effects of inertia that arise in connection with rotation and which are experienced as an outward force away from the center of rotation.

from Latin centrum, meaning "center", and fugere, meaning "to flee"

Page 107: 2014 SEPT - MECHANICS REG REVIEW.pdf

Centrifugal / Centripetal Force

FC = centrifugal/centripetal force

m = mass

v = velocity

r = radius

2

C

mVF

r

Page 108: 2014 SEPT - MECHANICS REG REVIEW.pdf

Guide Question

18. A 50,000 N car traveling with a speed of 150 km/hr rounds a curve whose radius is 150 m. Find the centrifugal force.

A. 65 kN

B. 38 kN

C. 70 kN

D. 59 kN

Page 109: 2014 SEPT - MECHANICS REG REVIEW.pdf

Banking of Highway Curves (Case I)

Car is rotating (circular) radius

of curvature r with velocity v.

MECH 312 RROCABERTE © 2013

N

W

Nμr

v

g

W

2

gr

2

W v2 g r

Fc=

f=μN

N

W

NW

Fc f

r

Page 110: 2014 SEPT - MECHANICS REG REVIEW.pdf

Banking of Highway Curves (Case II)

When v = vrated = 0 (car is not moving), upward frictional force is introduced to prevent skidding.

MECH 312 RROCABERTE © 2013

θ N

W

N W θ

N

N

fθ tan

θμ tan

f=μN

Page 111: 2014 SEPT - MECHANICS REG REVIEW.pdf

Banking of Highway Curves (Case III)

When v = vrated, no tendency to slip up or down the road (ideal banking of curve)

MECH 312 RROCABERTE © 2013

θ N

W

W v2 g r

Fc=

N W

Fc

θ

W

r

v

g

W

W

Fθ c

2

tan

gr

2

tan θ = ideal angle of banking

v = rated speed of the curve

Page 112: 2014 SEPT - MECHANICS REG REVIEW.pdf

Banking of Highway Curves (Case IV)

When v > vrated, downward frictional force f is introduced to prevent skidding.

MECH 312 RROCABERTE © 2013

θ R

W W v2 g r

Fc=

R W

Fc

W

r

v

g

W

W

Fθ c

2

tan Φ

N

θ φ

N

f

θ+φ

gr

2

tan Φ

Φtan

..

μ

fcμ

Page 113: 2014 SEPT - MECHANICS REG REVIEW.pdf

Banking of Highway Curves (Case V)

When v < vrated, upward frictional force f is introduced to prevent skidding.

MECH 312 RROCABERTE © 2013

θ

R

W W v2 g r

Fc= R W

Fc

W

r

v

g

W

W

Fθ c

2

tan Φ

N θ

φ

N

f θ-φ

gr

2

tan Φ

Φtan

..

μ

fcμ

Page 114: 2014 SEPT - MECHANICS REG REVIEW.pdf

19. A highway curve has a super elevation of 7 degrees. What is the radius of curvature of the curve such that there will be no lateral pressure between the tires and the roadway at a speed of 40 mph? A. 670 ft B. 770 ft C. 870 ft D. 970 ft

MECH 312 RROCABERTE © 2013

Page 115: 2014 SEPT - MECHANICS REG REVIEW.pdf

Example 5 20. The rated speed of a highway of 200 ft radius is 30 mph. If the coefficient of kinetic friction between the tires and the road is 0.60, what is the maximum speed at which a car can round the curve without skidding? A. 57.35 mph B. 102.34 mph C. 78.33 mph D. 23.83 mph

MECH 312 RROCABERTE © 2013

Page 116: 2014 SEPT - MECHANICS REG REVIEW.pdf

21. Find the angle of banking for a highway curve of 300 ft radius designed to accommodate cars travelling at 100 mph, if the coefficient of friction between the tires and the road is 0.6. What is the rated speed of the curve? A. 51.08 mph B. 45.334 mph C. 67.21 mph D. 55.9 mph

MECH 312 RROCABERTE © 2013

Page 117: 2014 SEPT - MECHANICS REG REVIEW.pdf

Test Yourself 1. vrated is used in what particular formula? 2. Formula for ideal banking of curves 3. Formula used when there is no frictional force

between the tires and the ground (no lateral pressure, no side thrust, etc.)

4. When a car is moving at its maximum, what is the formula?

5. When you consider the coefficient of friction between the tires and the road, what angle can we get? θ or Ф?

6. I want to know the coefficient of friction between my car’s tires and the ground. I parked my car on an inclined surface, θ from the horizontal. How do I determine for μ?

MECH 312 RROCABERTE © 2013

Page 118: 2014 SEPT - MECHANICS REG REVIEW.pdf

Answers to Test Yourself 1.tan θ = v2/gr 2.tan θ = v2/gr 3.tan θ = v2/gr 4.tan (θ + Ф) = v2/gr 5.Ф if car is moving not equal to the rated speed θ if car is not moving at all 6. μ = tan θ

MECH 312 RROCABERTE © 2013

Page 119: 2014 SEPT - MECHANICS REG REVIEW.pdf

Test Yourself Practice Problem: Determine the angle of super elevation for a highway curve of 600 ft radius so that there will be no side thrust for a speed of 45 mph. Ans. 12. 71°

MECH 312 RROCABERTE © 2013

Page 120: 2014 SEPT - MECHANICS REG REVIEW.pdf

UNIT 4

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

MECH 321: DYNAMICS OF RIGID BODIES (Summer 2013)

Page 121: 2014 SEPT - MECHANICS REG REVIEW.pdf

Angular Motion. Fixed Axis Rotation.

Fixed-axis rotation is defined as that motion of a rigid body in which the particles move in circular paths with their centers on a fixed straight line that is called the axis of rotation.

MECH 312 RROCABERTE © 2013

r

r

ωo

ωf

α θ = angular displacement, rad

ω0 = initial angular velocity, rad/s

ωf = final angular velocity, rad/s

α = angular acceleration, rad/s2

Uniform velocity:

α = 0, ωf = ω0

Starting from rest:

ω0 = 0

Stop at a point:

ωf = 0

θ

2

2

dt

θd

dt

ωdα

dt

θdω

Page 122: 2014 SEPT - MECHANICS REG REVIEW.pdf

Angular Motion. Fixed Axis Rotation.

Kinematic Differential Equations of Rotation

MECH 312 RROCABERTE © 2013

r ωo

ωf

α

θ

αra

dt

ωdr

dt

dv

ωrv

dt

θdr

st

ds

θrs

a vo

vf

s

2

22

ωra

r

ωr

r

va

αra

dt

dva

N

N

T

T

Page 123: 2014 SEPT - MECHANICS REG REVIEW.pdf

tαωω

αθωω

tαtωθ

of

of

o

2

2

1

22

2

Rotation with constant angular acceleration

For uniformly accelerated motion along a circular path:

atvv

asvv

attvs

of

of

o

2

2

1

22

2

αra

ωrv

θrs

Rectilinear Motion Rotation (Related by)

MECH 312 RROCABERTE © 2013

Page 124: 2014 SEPT - MECHANICS REG REVIEW.pdf

22. A flywheel of radius 14 inches is rotating at the rate of 1000 rpm. How fast does a point on the rim travel in ft/sec? A. 122.17 B. 1466.04 C. 100 D. 39.05

MECH 312 RROCABERTE © 2013

v=rω v=14in(1000rev/min)(1ft/12in)(2pi/1rev)(1min/60sec) v=122.17ft/s

Page 125: 2014 SEPT - MECHANICS REG REVIEW.pdf

23. When the angular velocity of a 4-ft diameter pulley is 3 rad/s, the total acceleration of a point on its rim is 30 fps2. Determine the angular acceleration of the pulley at this instant?

A. 9 rad/s2

B. 12 rad/s2

C. 15 rad/s2

D. 14 rad/s2

MECH 312 RROCABERTE © 2013

2

222

2

/12 sradα

αra

aaa

ωra

T

nt

N

Page 126: 2014 SEPT - MECHANICS REG REVIEW.pdf

24.. A flywheel rotating at 200 rev/min slows down at a constant rate of 2 rad/s2. How many revolutions does it make in the process?

A. 10.47 B. 17.5

C. 109.7 D. 62.83

There’s no other way but up!

Page 127: 2014 SEPT - MECHANICS REG REVIEW.pdf

Work-Energy Theorem

Rowel Allan Rocaberte, REE, ECE

[email protected]

+63926 – 740 – 1530

Page 128: 2014 SEPT - MECHANICS REG REVIEW.pdf

Work – energy required to move an object by a distance

Potential Energy – energy possessed by an object by virtue of its motion (energy at rest), PE = mgh

Kinetic Energy – energy possessed by an object by virtue of its motion (energy in motion), KE = ½ mv2

Power – rate at which energy/work is transferred or consumed

Recall:

Fvdt

dsF

time

WorkP

Page 129: 2014 SEPT - MECHANICS REG REVIEW.pdf

Work – product of the component of force in a direction of displacement

Recall:

θ θ

P

θPsWork cos

+W if direction of W is in the direction of displacement -W if direction of W is opposite the direction of displacement

Page 130: 2014 SEPT - MECHANICS REG REVIEW.pdf

• Relates the force, displacement and velocity in a given system

• Removes the analysis of internal forces like tension

Work-Energy Method

Principle: The work done in a translating body is equal to the

sum of the change in kinetic energy of the body.

ifnet KEKEKEW

Page 131: 2014 SEPT - MECHANICS REG REVIEW.pdf

Derivation of Formula

ds

dvva

dvvdsa

ag

WF

KEsF

vvmsF o

22

2

1

22

00

2o

v

v

s

vvg

WsF

dvvg

WdsF

ds

dvv

g

WF

resultant work

change in kinetic energy

Page 132: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: Suppose a 30.0-kg package on the roller belt conveyor system is moving at 0.500 m/s. What is its kinetic energy?

Ans. 3.5 J

KE = 1/2mv 2 KE=0.5(30.0 kg)(0.500 m/s) 2

KE=3.75 kg⋅m2/s 2 =3.75 J.

Page 133: 2014 SEPT - MECHANICS REG REVIEW.pdf

Practice Problem: Suppose that you push on the 30.0-kg package with a constant force of 120 N through a distance of 0.800 m, and that the opposing friction force averages 5.00 N. (a) Calculate the net work done on the package. (b) Solve the same problem as in part (a), this time by finding the work done by the applied force. Find the work done by the friction.

Ans. (a) 92.0 J; (b) 96.0 J; (c) -4.0 J

(b) The applied force does work: Wapp = Fappdcos(0º)=Fappd = (120 N)(0.800 m) = 96.0 J

(c) So the amounts of work done by gravity, by the normal force, by the applied force, and by friction are, respectively Wgr = 0 Wn = 0 Wapp = 96.0 J Wfr= −4.00 J The total work done: W total= Wgr + Wn + Wapp + Wfr = 92.0

Page 134: 2014 SEPT - MECHANICS REG REVIEW.pdf

Energy Stored in a Spring

F = axial force

x = elongation

k = spring constant

2

2

1

2

1kxEFxE springspring

Page 135: 2014 SEPT - MECHANICS REG REVIEW.pdf

25. A large coil spring with a spring constant k = 120 N/m is elongated, within its elastic range by 1 m. Compute the stored energy of the spring in N-m.

A. 60

B. 40

C. 20

D. 120

Page 136: 2014 SEPT - MECHANICS REG REVIEW.pdf

26. The combined mass of car and passengers travelling at 72 km/hr is 1500kg. Find the kinetic energy of this combined mass.

A. 300kJ

B. 330kJ

C. 305kJ

D. 310kJ

K=mv2 = (1500kg)(72km/hr)2 (1000m/km)2 2k (2)(1kg-m/N-sec2 )(3000 sec/hr)2 = 300,000 J or 300 kJ

Page 137: 2014 SEPT - MECHANICS REG REVIEW.pdf

27. A Foucault pendulum swings to 3.0 in above the ground at the highest points and is practically touching the ground at the lowest point. What is the maximum velocity of the pendulum?

A. 4 ft/s C. 5 ft/s

B. 2 ft/s D. 10 ft/s

lost gainedPE =KE

v = 2gh

Page 138: 2014 SEPT - MECHANICS REG REVIEW.pdf

UNIT 7

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

MECH 321: DYNAMICS OF RIGID BODIES (1st Sem 2013-2014)

Front slide photo taken from http://origami-blog.origami-kids.com/paper-airplanes-glossary-of-terms.htm

Page 139: 2014 SEPT - MECHANICS REG REVIEW.pdf

Definition

Momentum

- Measure of the motion of a body

- Quantity of motion that an object has

- Product of mass and velocity

Impulse

- Produced when force is applied over time periods

- Product of force and the time

MECH 312 RROCABERTE © 2013

mvP

FtI

Page 140: 2014 SEPT - MECHANICS REG REVIEW.pdf

Impulse-Momentum Theorem

Impulse equals the change in momentum

MECH 312 RROCABERTE © 2013

12 vvmFt

dt

dv

g

WF

dt

dva

ag

WF

o

v

v

t

vvg

WtF

dvg

WdtF

dvg

WdtF

o

0

Page 141: 2014 SEPT - MECHANICS REG REVIEW.pdf

Law of Conservation of Momentum

Special Case (when P and KE are conserved) :

u2 – u1 relative velocity of separation after collision

v1 – v2 relative velocity of approach before collision

MECH 312 RROCABERTE © 2013

collisionaftercollisionbefore PP

1221 uuvv D6.

Page 142: 2014 SEPT - MECHANICS REG REVIEW.pdf

Coefficient of Restitution

The coefficient of restitution (e), or bounciness

of an object is a fractional value representing the

ratio of relative velocities after and before an impact.

An object with an e of 1 collides elastically, while an object with an e < 1 collides inelastically.

MECH 312 RROCABERTE © 2013

Coefficient of Restitution

Collision Remark

e = 1 Perfectly elastic P and KE is conserved

e < 1 Inelastic collision P is conserved; KE is not conserved

e = 0 Perfectly plastic P and KE is not conserved (e.g. colliding particles stick together)

21

12

vv

uue

Page 143: 2014 SEPT - MECHANICS REG REVIEW.pdf

21

12

vv

uue

1

2

tan

tan

e

o

r

h

he

Page 144: 2014 SEPT - MECHANICS REG REVIEW.pdf

Sign Convention:

Before Collision

After collision

Law of Conservation of Momentum

Loss in Kinetic Energy

MECH 312 RROCABERTE © 2013

100%

initial

initialfinal

loss

initialfinalloss

KE

KEKEKE

KEKEKE

m1 m2

m1 m2

v1 v2

u2 u1

+v -v

22112211 umumvmvm

Page 145: 2014 SEPT - MECHANICS REG REVIEW.pdf

28. If the coefficient of restitution is zero, the impact is __________.

A. partially plastic

B. perfectly plastic

C. perfectly elastic

D. partially elastic

Page 146: 2014 SEPT - MECHANICS REG REVIEW.pdf

Guide Question

29. A ball is dropped from a height of 20 m upon a stationary slab. If the coefficient of restitution is 0.40, how high will the ball rebound?

A. 3.2 m

B. 4.6 m

C. 5.2 m

D. 8.0 m

Page 147: 2014 SEPT - MECHANICS REG REVIEW.pdf

30. The 10 kg and 20 kg bodies are approaching each other with the velocities shown. If e = 0.60, what will be the velocity of each body directly after impact? (a) u1 = -13.33 m/s, u2 = 10 m/s (b) u1 = 6.0 m/s, u2 = 7.5 m/s (c) u1 = 10.25 m/s, u2 = 10 m/s (d) u1 = -13.33 m/s, u2 = 16.7 m/s

MECH 312 RROCABERTE © 2013

21

12

vv

uue

signstheofnote

umumvmvm 22112211

Page 148: 2014 SEPT - MECHANICS REG REVIEW.pdf

31. A 200-lb block in contact with the ground is acted upon by a horizontal force equal to 100 lb. The coefficient of kinetic friction is 0.20. In what time will the velocity of the block be increased from 4 fps to 10 fps?

A. 0.621 s

B. 5.1 sec

C. 1.23 sec

D. 8 ms

MECH 312 RROCABERTE © 2013

sec621.0

12

t

vvmtF

Page 149: 2014 SEPT - MECHANICS REG REVIEW.pdf

32. A gun is shot in a 0.50 kN block which is hanging from a rope of 1.8 m long. The weight of the bullet is equal to 5 N with a muzzle velocity of 320 m/s. How high will the block swing after it was hit by the bullet?

A. 0.51 m

B. 0.53 m

C. 0.32 m

D. 0.12 m

m1v1 + m2v2 = m1u1 + m2u2

m1v1 + m2v2 = mTu

500(0) + (5/9.81)(320) = (500+5)/9.81 x u u = 3.168 m/s PE = KE mgh = mu2/2 h = u2/2g h = 3.1682/(2x9.81) = 0.512 m

Page 150: 2014 SEPT - MECHANICS REG REVIEW.pdf

UNIT 8

Rowel Allan Rocaberte, REE, ECE [email protected]

+63926 – 740 – 1530

MECH 321: DYNAMICS OF RIGID BODIES (Summer 2013)

Page 151: 2014 SEPT - MECHANICS REG REVIEW.pdf

Frequency of SHM

Simple

pendulum

Conical

pendulum

L

h

Page 152: 2014 SEPT - MECHANICS REG REVIEW.pdf

Frequency of SHM

Helical

spring

in SHM

m

k = spring constant

m = mass

a= acceleration

x = displacement

General

formula

Page 153: 2014 SEPT - MECHANICS REG REVIEW.pdf

33. Calculate the period of a simple pendulum connected to a string of length 2 meters.

A. 2.1 sec C. 1.9 sec

B. 1.7 sec D. 2.8 sec

Page 154: 2014 SEPT - MECHANICS REG REVIEW.pdf

34. What is the frequency of a 0.6-kN/m helical spring in simple harmonic motion if a body of 3 kg is attached to its end.

A. 1.75 Hz

B. 2.0 Hz

C. 2.25 Hz

D. 1.9 Hz