lecture 3: rigid body dynamics - brown ... - brown...

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Lecture 3: rigid body dynamics kinematics example: rolling no slip rotational equation of motion mass moment of inertia solving rigid body dynamics problems dynamics example: pulley with mass Thursday, April 11, 13

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Page 1: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Lecture 3: rigid body dynamics

• kinematics example: rolling no slip• rotational equation of motion• mass moment of inertia• solving rigid body dynamics problems• dynamics example: pulley with mass

Thursday, April 11, 13

Page 2: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Rigid Body Kinematics

• Useful Shortcuts for 2D planar motion

aA = aB + (↵⇥ rA/B) + (! ⇥ (! ⇥ rA/B))vA = vB + (! ⇥ rA/B)

↵ = ↵k! = !kr = r

x

i + ry

j

! ⇥ r = �ry

!i + rx

!j↵⇥ r = �r

y

↵i + rx

↵j

! ⇥ (! ⇥ r) = �rx

!2i� ry

!2j

Thursday, April 11, 13

Page 3: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Rigid Body Dynamics

F = ma =d(mv)

dt

Linear Motion:sum of the forces is the time rate of change of linear momentum

Works for particles - and also works for rigid bodies if the acceleration is at the center of mass!

F = maG

Thursday, April 11, 13

Page 4: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Rigid Body Dynamics

Rotational Motion:

sum of the moments is the time rate of change of angular momentum

MG =d(HG)

dt= HG

about the center of mass

Thursday, April 11, 13

Page 5: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Rigid Body Dynamics

Rotational Motion:

sum of the moments is the time rate of change of angular momentum

MG =d(HG)

dt= IG↵

Mass Moment of Inertia:

“Rotational Inertia”

Resistance to angular acceleration

IG =X

i

(mir2i ) =

Z

V(⇢r2)dV

Thursday, April 11, 13

Page 6: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Mass Moment of InertiaL

m Two spherical masses connected by a massless bar

m

zsolid cylinder length L radius R, rotating around z-axis

thin plate, height b, length c, rotating around y-axis

y

Thursday, April 11, 13

Page 7: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Thursday, April 11, 13

Page 8: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Thursday, April 11, 13

Page 9: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Parallel Axis TheoremG O

d

IO = IG + md2

object rotating around axis “O” NOT through the CG

Find parallel axis through CG

IG can read from tables

Thursday, April 11, 13

Page 10: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

Composite BodiesO

d1

d2

d2

1 2 3

IO = IG1 + m1d21 + IG2 + m2d

22 + IG3 + m3d

23

IG can read from tables

Thursday, April 11, 13

Page 11: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

rigid body dynamics problems:2D planar motion

• Free Body Diagram!• 3 equations of motion:

• problem constraints• mass moment of inertia calculation • can we solve? if not, need more eqns:• kinematics equations: connection between

Fx

= max

Fy

= may

Mz

= I↵

↵, ! AND v, a

Thursday, April 11, 13

Page 12: Lecture 3: rigid body dynamics - Brown ... - Brown Universitybrown.edu/.../Notes/JF_Rigid_Body_Lectures/Lecture3... · Lecture 3: rigid body dynamics • kinematics example: rolling

refer to 2012 HW#7 for more details and solution

Thursday, April 11, 13