chapter 13 dynamics. chapter 3 newton’s law newton's law of inertia a body, not acted on by...

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Chapter 13 Dynamics

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Page 1: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Chapter 13

Dynamics

Page 2: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Chapter 3 Newton’s Law

Page 3: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in

uniform motion. NEWTON'S LAW OF MOTION

Moving an object with twice the mass will require twice the force.

Force is proportional to the mass of an object and to the acceleration (the change in velocity).

F=ma.

Page 4: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 5: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

W = m*g

Page 6: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Fnet = F = T1 + T2 + T3 = 0

Page 7: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

x- and y-components:T1x = - T1 cos 37o = - 0.8 T1T1y = T1 sin 37o = 0.6 T1T2x = T2 cos 53o = 0.6 T2T2y = T2 sin 53o = 0.8 T2

Page 8: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Solve for tension T1 and T2.Fnet,x = F x = T1 x + T2 x + T3 x = 0T1 x + T2 x + T3 x = 0- 0.8 T1 + 0.6 T2 + 0 = 0

T1 = 0.75 T2

Page 9: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Dynamics

M1: up as positive:Fnet = T - m1*g = m1 a1

M2: down as positive.Fnet =  F = m2*g - T = m2 a2

3. Constraint equation:a1 = a2 = a

Page 10: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Equations

From previous:T - m1*g = m1 a

T = m1 g + m1 a Previous for Mass 2:m2*g - T = m2 a

Insert above expr. for Tm2 g - ( m1 g + m1 a ) = m2 a

( m2 - m1 ) g = ( m1 + m2 ) a( m1 + m2 ) a = ( m2 - m1 ) g

a = ( m2 - m1 ) g / ( m1 + m2 )

Page 11: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Rules1. Free-Body Analysis, one for each mass + Newton’s Law

3. Algebra:Solve system of equations for all unknowns

2. Constraint equation(s): Define connections.You should have as many equations as Unknowns.COUNT!

Page 12: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

0 = 30 0

g

i

J

m

M*g

M*g*sin

-M*g*cosj

Mass m rests on the 30 deg. Incline as shown. Step 1: Free-Body Analysis. Best approach: use coordinates tangential and normal to the path of motion as shown.

Page 13: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Mass m rests on the 30 deg. Incline as shown. Step 1: Free-Body Analysis.

Step 2: Apply Newton’s Law in each Direction:

0 = 30 0

g

i

J

m

M*g

M*g*sin

-M*g*cosj

xmxForces *i*sin*g*m)_(

)_(0j*cos*g*m-N )_( onlystaticyForces

N

Page 14: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Friction F = k*N:Another horizontal

reaction is added in negative x-direction.

0 = 30 0

g

i

J

m

M*g

M*g*sin

-M*g*cosj

xmNkxForces *i*)*sin*g*m()_(

)_(0j*cos*g*m-N )_( onlystaticyForces

N k*N

Page 15: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Midterm 1 :Some suggestions

•Systematic work: it takes practice, lots of it.

•Passive understanding is good, yet you still must train yourself through active practice.

•It’s all mathematical: Practice calculus and analytical geometry!

Page 16: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Midterm 1:Suggestions cont’d

•‘Deep Thinking 1’: Map the solution path BEFORE starting the analysis.

‘Deep Thinking 2’: Select the laws you will use.

•‘Deep Thinking 3’: Map out the Connections between the laws that will lead to the answer.

Page 17: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Preparing for Exam 1

•Modeling: Free-Body Analysis

•Laws and Definitions: Laws of Kinematics, Terms such as , Coriolis accel, Moving Frames of Ref.

•Seek to understand the concepts

•Practice problem solving. Copying the homework gives you an illusion and useless points

Page 18: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Multiple Masses A and B move in i and j-directions.

Steps: 1. Write Newton for

each Mass.2. Constraint equation

connects both masses. Here:

30 deg.

g

x

y60 deg.

vA = - vB

Page 19: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

fig_03_007

Newton’s Law for Rotation

rramF *

amF *

Page 20: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 21: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 22: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 23: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 24: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 25: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 26: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION
Page 27: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Step 1: Free-Body Analysis

Page 28: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Step 2: Newton in radial and tangential directions

Page 29: Chapter 13 Dynamics. Chapter 3 Newton’s Law NEWTON'S LAW OF INERTIA A body, not acted on by any force, remains in uniform motion. NEWTON'S LAW OF MOTION

Rotation Kinematics

Similar to translation:

dt*

dt*

and dd **