chapter 3 rigid bodies: equivalent system of forces
TRANSCRIPT
CHAPTER 3
RIGID BODIES: EQUIVALENT SYSTEM OF FORCES
Objectives• 3.1 Introduction • 3.2 External and Internal Forces• 3.3 Principle of Transmissibility• 3.4 Vector Product of two vectors• 3.5 Vector Product expressed in terms of rectangular components• 3.6 Moment of a Force about a point• 3.7 Varignon’s Theorem• 3.8 Rectangular components of the moment of the force• 3.9 Scalar Product of 2 vectors• 3.10 Mixed triple product of 2 vectors• 3.11 Moment of a force about a given axis• 3.12 Moment of a couple• 3.13 and 3.14 Equivalent and Addition of Couples• 3.15 Couples represented by vectors• 3.16 Resolution of a given force into a force at O and a couple• 3.17 Resolution of a system of forces to one force and one couple
So far, we have reviewed• Fundamental Principles:
– Parallelogram law– Newton’s laws– Principle of transmissibility
• Assumption: A rigid body could be treated as a single particle (not always true)
In this Chapter you will learn• The effect of forces exerted on a rigid body and how to
replace a given system of forces by a simpler equivalent system.
3.2 External and Internal Forces
• External Forces: – responsible for the external behavior of the
rigid bodies.– cause the rigid bodies to move or ensure that
they remain at rest.
• Internal Forces:– hold together the particles or parts forming the
rigid body.
Examples of external Forces
FBD
W
R1 R2
W: weight of the truck. Point of application center of gravity.
R1 and R2: reactions by the ground.
F: force of exertion, point of application truck’s bumper. It causes translation
F
3.3 Principle of transmissibility, equivalent forces
• Forces acting on a particle: vectors with a well defined point of application, called bound or fixed vectors.
• Forces acting on a rigid body: vectors whose point of application of the force doesn’t matter, as long as the line of action remains unchanged, called sliding vectors.
Principle of transmissibility
=F
F’
F and F’ have the same effect if their magnitude , direction and line of action are the same. Based on experimental evidence.
Principle of transmissibility
W
R1 R2
Conditions of motion are unaffected. F and F’ are equivalent
W
=
R1 R2
F F’
3.4 Vector product of 2 vectors• Vector product of 2 vectors is defined as a vector V,
which satisfies the following:– 1) Line of action of V is perpendicular to the plane
containing P and Q.
– 2) The magnitude of V is:
V=P Q sin – 3) The direction of V is obtained by the right hand rule.
Q
P
V=PxQ
Vector product
• The magnitude of V is also equal to the area of the parallelogram that has P and Q for sides.
Q
P
VV=PxQ
Q’
A1
V=PxQ’
V=P x Q=P x Q’
A2
Other properties of vector product:
• Commutative:
• Distributive:
• Associative Property:
NO Q x P P x Q
YES P x (Q1+Q2) = P x Q1 +P x Q2
NO(P x Q) x S P x (Q x S)
Vector expressed in terms of rectangular components
• Vector product of any 2 units vectors: i, j, k
• i x j= k
• j x i= -k
• j x k= i
• k x j= -i
• k x i= j
• i x k= -j
• i x i= 0, j x j= 0, k x k= 0
x
y
z
ij
k
i
j
k
(+):CCW
(-):CW
• We can express the vector product of two given vectors P and Q in terms of rectangular components:
• V=P x Q=(Pxi+Pyj+Pzk) x (Qxi+Qyj+Qzk)
• Using distributive property and the products of unit vectors:
• V=(PyQz-PzQy)i + (PzQx-PxQz)j+(PxQy-
-PyQx)k
• Vx=(PyQz-PzQy)
• Vy=(PzQx-PxQz)
• Vz=(PxQy-PyQx)
The right hand members represent the expansion of a determinant.
V=i j kPx Py Pz
Qx Qy Qz
i j k i jPx Py Pz Px Py Qx Qy Qz Qx Qy
(+)(-)
3.6 Moment of a Force around a point
A
F
r
M0
O
d
•The effect of the force F on the rigid body depends on its:•Magnitude•Direction•Point of application (A)
•Position of A: represented by r•r and F define a plane.•M0= r Fsin = Fd , where d= perpendicular distance from O to the line of action of F.Moment of F around O: M0= r x F, M0 is perpendicular to the
plane containing O and F The sense of F is defined by the right hand rule.
Units of Moment
• SI: Nm
• US Units: lb ft or lb in
3.8 Rectangular Components of the moment of a force
• We restate the principle of transmissibility as:
• Two forces F and F’ are equivalent if, only if, :– they are equal (=magnitude, = direction)– And have equal moment about a given point O
– F=F’ M0=M0’
3.7 Varignon’s Theorem
Moment of the resultant Sum of the moments
of several forces = of each force around
the same point O
r x (F1+F2+……)= r x F1+ r x F2+…
3.8 Rectangular Components of the moment of a Force
• We can simplify the calculation of the moment of a force by resolving the force and the position vector into components.
r = x i +y j +z k
F=Fx i +Fy j +Fz k
M0= r x F
Rectangular components of the moment of a force
i j k i jx y z x y Fx Fy Fz Fx Fy
(+)(-)
M0=(y Fizz-z Fy) i+ (z Fx-x Fz) j+ (xFy- y Fx) k
Mx=(y Fz-z Fy) My=(z Fx-x Fz) Mz=(xFy- y Fx)
Sample Problem 3.1
• A vertical force of 100 lb is applied to the end of the rod bar which is attached to a shaft at O. Determine:– A) Moment of a 100 lb force about O– B) The horizontal force applied at A which
creates the same moment about O.– C)The smallest force at A which creates the
same moment about O.
3.9 Scalar product of 2 vectors
• The scalar product, (or dot product) of two vectors is defined as:
P Q= P Q cos (scalar)
• Satisfies: – Commutative Property: P Q= Q P
– Distributive Property: P (Q1 + Q2)= P Q1+P Q2
Scalar product of 2 vectors
• The scalar product of 2 vectors P and Q can be expressed as:
• P Q=(Pxi + Pyj + Pzk) (Qxi + Qyj + Qzk)• And
i j= 0, j k= 0, k i= 0i i= 1, j j= 1, k k= 1
• Therefore:• P Q = PxQx + PyQy + PzQz
Special Case
• P=Q
• P P = Px Px + PyPy + PzPz
=P2
Applications
• 1) To determine the angle between two vectors
• P Q cos =PxQx + PyQy + PzQz
• Solving for cos …
• cos =
PxQx + PyQy + PzQz
P Q
2nd Application: Projection of a vector in a given axis
O
Laxis
P
The projection of P along the axis OL is defined as a scalar:POL=P cos (+) if OA has the
same sense as OL (axis) (-) if OA has the
opposite sense as OL (axis)QA
•Consider Q directed along the axis OL:
POL
= POL Q• P Q= P Q cos P Q= POL QPOL= P Q
Q
x
y
z
P Q Q
POL=
POL= P , POL= Px x+Py y+Pz z
3.10 Mixed triple product of 3 vectors
• Mixed triple product=S (P x Q)
• Geometrically:
• Mixed triple product=Volume of the parallelepiped having S, P and Q for sides
(Scalar expression)
S
P
Q
(+) If the vectors are read ccw order or circular permutation
(-) cw direction
S
P
Q
Mixed triple product in terms of rectangular components
S (P x Q) = Sx(Py Qz-Pz Qy) + Sy(Pz Qx-Px Qz) + Sz(PxQy- -Py Qx)
In compact form:
S (P x Q)=
Sx Sy Sz Px Py Pz
Qx Qy Qz
Application of triple product
3.11 Moment of a Force around a given axis
• Given a force, a position vector and a moment :
F
r
M0
O
L
A(x,y,z)
axis•We define moment MOL of F about OL: projection of the moment M0 onto the axis OL.•Projection of a vector onto an axis
POL= P ,
MOL= M0
(r x F)
MOL= (r x F)
Mixed Triple Product
In determinant form:
MOL=
x y z x y z Fx Fy Fz
Where x , y , z are direction cosines of OLx, y, z are coordinates of point of application of
FFx, Fy, Fz are components of F
Moment MOL:
Measures the tendency of F to impart to the rigid body rotation about a fixed axis OL
What is the difference between MOL and M0?
How is the moment of a force applied at A, about an axis, which does not pass through the origin obtained?
By choosing an arbitrary point B on the axis
FB
A
rA/B=rA-rB
O
L
Determine the projection on the axis BL of MB of F about B.
MBL= MB BL = BL(rA/B x F)
Moment MBL
FB
A
rA/B=rA-rB
O
L
MBL=
x y z xA/B yA/B zA/B Fx Fy Fz
Where xA/B=xA-xB, yA/B= yA-yB, zA/B= zA-zB
The result of the moment of F about the axis L is independent of the choice of the point B on the given axis.
Sample problem 3.5
• A force P acts on a cube of side a. Determine the moment of P:– a) about A– b) about AB– c) about AG
3.12 Moment of a couple
• Couple: Two forces F and -F having the same magnitude, parallel lines of action and opposite sense. The forces tend to make the body on which they act rotate.
-F
F
Being rA and rB the position vectors of the points of application of F and -F.
The sum of the moments of F and -F about O M=rA x F + rB x (-F)= (rA-rB) x F
M = r x FM= moment of a couple. It’s perpendicular to the plane containing the 2 forces. Its magnitude isIts sense is defined by the right hand rule
M=r F sin = F d
rA
FrB
-F
O
r
M
A
B
d
3.13 Equivalent Couples
• Two couples that have the same moment M are equivalents.
20 lb20 lb
6 inch
4 inch
4 inch
6 inch
4 inch
4 inch
30 lb
30 lb=
Equivalent systems
3.14 Addition of Couples
• Given two systems of couples: – F1 and -F1– F2 and -F2
• M1=r x F1
• M2=r x F2
• Resultant Moment M=M1+M2
3.15 Couples can be represented by vectors
• Instead of drawing actual forces:
• Draw an arrow equal in magnitude and direction to the moment M of the couple
M
“couple vector”
-F
F
Ox
y
z
• Couple vector:– is a free vector (point of application can be moved)
– can be resolved into components Mx, My, Mz
M
“couple vector”
Ox
y
z
3.16 Resolution of a given force into a force at O and a couple
• Consider F
F
OAr
•We’d rather have a force acting at O
F
- Fr
F F
O O
M0
• add 2 forces at O Mo=r x F
Force couple system
= =
F
OAr
F
- Fr
F F
O O
M0
Force couple system
= =
Conclusion: Any F acting on a rigid body can be moved to
an arbitrary point O provided that a couple is added whose moment is equal to the moment of F about O
F
OAr
F
O
M0
=
If F is moved from A to O’
A
O’s’
rr’
F
O
M0
A
O’s’
rr’=
•To move F from O to O’, it’s necessary to add a couple vector.
Mo’= r’ x F= (r + s) x F = (r x F) + (s x F)
Mo’ = MO + (s x F)
Sample problem 3.6
• Determine the components of a single couple equivalent to the couples shown in the figure (page 113).
3.17 Resolution of a system of forces to one force and a couple
• Any system of forces can be reduced to an equivalent force-couple system acting at a point O.
F1
F2
F3
M1
M2
M3
R
MoR
=
R= F, MoR= Mo= (r x F)
THE END…..
…….FOR CHAPTER 3