kinetics of particles impulse and momentum
DESCRIPTION
Kinetics of Particles Impulse and Momentum. Linear Impulse and Linear Momentum. Consider the general curvilinear motion in space of a particle of mass m , where the particle is located by its position vector measured from a fixed origin O. - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/1.jpg)
![Page 2: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/2.jpg)
Consider the general curvilinear motion in space of a particle of mass m, where the particle is located by its position vector measured from a fixed origin O.
r
The velocity of the particle is is tangent to its path. The resultant force of all forces on m is in the direction of its acceleration .
rv
va
We may write the basic equation of motion for the particle, as
vmamF
or
GGdtdvm
dtdvmF
Where the product of the mass and velocity is defined as the linear momentum of the particle. This equation states that the resultant of all forces acting on a particle equals its time rate of change of linear momentum.
F
vmG
![Page 3: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/3.jpg)
In SI, the units of linear momentum are seen to be kg.m/s, which also equals N.s.
Linear momentum equation is one of the most useful and important relationships in dynamics, and it is valid as long as mass m of the particle is not changing with time.
We now write the three scalar components of linear momentum equation as
xx GF yy GF zz GF
These equations may be applied independently of one another.
vm
![Page 4: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/4.jpg)
The Linear Impulse-Momentum Principle
All that we have done so far is to rewrite Newton’s second law in an alternative form in terms of momentum. But we may describe the effect of the resultant force on the linear momentum of the particle over a finite period of time simply by integrating the linear momentum equation with respect to time t. Multiplying the equation by dt gives , which we integrate from time t1 to time t2 to obtain
momentumlinearinchange
G
G
impulselinear
t
t
GGGGddtF 12
2
1
2
1
GddtF
Here the linear momentum at time t2 is G2=mv2 and the linear momentum at time t1 is G1=mv1. The product of force and time is defined as the linear impulse of the force, and this equation states that the total linear impulse on m equals the corresponding change in linear momentum of m.
dtGdF
![Page 5: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/5.jpg)
Alternatively, we may write
21 GdtFG
I
which says that the initial linear momentum of the body plus the linear impulse applied to it equals its final linear momentum.
m v1+ =
11 vmG
dtF
22 vmG
![Page 6: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/6.jpg)
The impulse integral is a vector which, in general, we may involve changes in both magnitude and direction during the time interval. Under these conditions, it will be necessary to express and in component form and then combine the integrated components. The components become the scalar equations, which are independent of one another.
F
G
xxxxx
t
tx GGGmvmvdtF 12
2
1
12
yyyyy
t
ty GGGmvmvdtF 12
2
1
12
zzzzz
t
tz GGGmvmvdtF 12
2
1
12
![Page 7: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/7.jpg)
There are cases where a force acting on a particle changes with the
time in a manner determined by experimental measurements or by
other approximate means. In this case, a graphical or numerical
integration must be performed. If, for example, a force acting on a
particle in a given direction changes with the time as indicated in the
figure, the impulse, , of this force from t1 to t2 is the shaded
area under the curve.
dtFt
t2
1
![Page 8: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/8.jpg)
Conservation of Linear Momentum
If the resultant force on a particle is zero during an interval of time, its linear momentum G remains constant. In this case, the linear momentum of the particle is said to be conserved. Linear momentum may be conserved in one direction, such as x, but not necessarily in the y- or z- direction.
210 GGG
21 vmvm
This equation expresses the principle of conservation of linear momentum.
![Page 9: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/9.jpg)
PROBLEMS
1. The 200-kg lunar lander is descending onto the moon’s surface with a velocity of 6 m/s when its retro-engine is fired. If the engine produces a thrust T for 4 s which varies with the time as shown and then cuts off, calculate the velocity of the lander when t=5 s, assuming that it has not yet landed. Gravitational acceleration at the moon’s surface is 1.62 m/s2.
![Page 10: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/10.jpg)
SOLUTION
smvv
v
vmg
mvmvFdt
vsmg
stsmvkgm
/ 1.29.36
620016008001620
62002)800(221)800()5(
? , / 62.1
, 5 , / 6 , 200
2
2
2
2
12
22
1
mg
motion
T+
![Page 11: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/11.jpg)
PROBLEMS
2. The 9-kg block is moving to the right with a velocity of 0.6 m/s on a horizontal surface when a force P is applied to it at time t=0. Calculate the velocity v of the block when t=0.4 s. The kinetic coefficient of friction is k=0.3.
![Page 12: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/12.jpg)
SOLUTION
smvv
vdtdtdt
mvmvFdt
directionxin
NFNN
mgNF
tt
t
t
t
kf
y
/823.14.59)4.0(49.26)2.0(36)2.0(72
)6.0(9)3.88(3.03672
)3.88(3.0 3.88)81.9(9
0 0
22
24.0
0
4.0
2.0
2.0
0
10
2
22
1
1
motionx
y
PW=mg
N Ff=kN
![Page 13: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/13.jpg)
PROBLEMS
3. A tennis player strikes the tennis ball with her racket while the ball is still rising. The ball speed before impact with the racket is v1=15 m/s and after impact its speed is v2=22 m/s, with directions as shown in the figure. If the 60-g ball is in contact with the racket for 0.05 s, determine the magnitude of the average force R exerted by the racket on the ball. Find the angle made by R with the horizontal.
![Page 14: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/14.jpg)
68.8 tan 02.43
49.6 325.005.0
10sin1506.020sin2206.0)81.9(06.0
53.42 127.205.0
10cos1506.020cos2206.0
05.00
05.0
0
10
2
05.00
10
2
x
y
yy
y
y
t
yy
xx
x
x
t
xx
RR
NR
NRR
ttR
mvmvdtF
NRR
tR
mvmvdtF
SOLUTION
Rx
RyR
W=mg
Rx
RyR
in x direction
in y direction
x
1v
2v
10°20°
xv1
yv1
xv2yv2
y
![Page 15: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/15.jpg)
PROBLEMS
4. The 40-kg boy has taken a running jump from the upper surface and lands on his 5-kg skateboard with a velocity of 5 m/s in the plane of the figure as shown. If his impact with the skateboard has a time duration of 0.05 s, determine the final speed v along the horizontal surface and the total normal force N exerted by the surface on the skateboard wheels during the impact.
![Page 16: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/16.jpg)
PROBLEMS(mB+mS)g
N
y
x
s/m.vvcos
vmmvmvm SBSxSBxB
853540030540
Linear momentum is conserved in x-direction;
kNNorNN
N
dtgmmNvmvm SBSySByB
44.22440005.081.94505.0030sin540
005.0
0
in y direction
![Page 17: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/17.jpg)
r
In addition to the equations of linear impulse and linear momentum, there exists a parallel set of equations for angular impulse and angular momentum. First, we define the term angular momentum. Figure shows a particle P of mass m moving along a curve in space. The particle is located by its position vector with respect to a convenient origin O of fixed coordinates x-y-z.
y
![Page 18: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/18.jpg)
The velocity of the particle is , and its linear momentum is . The moment of the linear momentum vector about the origin O is defined as the angular momentum of P about O and is given by the cross-product relation for the moment of a vector
GrvmrHo
The angular momentum is a vector perpendicular to the plane A defined by and . The sense of is clearly defined by the right-hand rule for cross products.
rv vmG
vm
OH
r
v OH
![Page 19: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/19.jpg)
The scalar components of angular momentum may be obtained from the expansion
kyvxvmjxvzvmizvyvmvvvzyxkji
mH xyzxyz
zyx
o
In SI units, angular momentum has the units kg.m2/s =N.m.s.
so that
yzox zvyvmH zxoy xvzvmH xyoz yvxvmH
vmrHo
![Page 20: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/20.jpg)
If represents the resultant of all forces acting on the particle P, the moment about the origin O is the vector cross product
F
vmrFrM o
oM
We now differentiate with time, using the rule for the differentiation of a cross product and obtain
vmrHo
oM
amrmro vmrvmrvmr
dtdH
0
The term is zero since the cross product of parallel vectors is zero.
vmv
![Page 21: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/21.jpg)
The scalar components of this equation is
oxox HM oyoy HM ozoz HM
Substitution into the expression for moment about O gives
oo HM
![Page 22: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/22.jpg)
The Angular Impulse-Momentum Principle
To obtain the effect of the moment on the angular momentum of the particle over a finite period of time, we integrate from time t1 to t2.
oo HM
ooo
H
H
o
t
to HHHHddtM
o
o
12
2
1
2
1
o
momentumangularinchange
impulseangulartotal
t
to HvmrvmrdtM
1122
2
1
or
The total angular impulse on m about the fixed point O equals the corresponding change in angular momentum of m about O.
21
2
1
o
t
too HdtMH
Alternatively, we may write
![Page 23: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/23.jpg)
Plane-Motion Application
Most of the applications can be analyzed as plane-motion problems where moments are taken about a single axis normal to the plane motion. In this case, the angular momentum may change magnitude and sense, but the direction of the vector remains unaltered.
1122
12
2
1
2
1
sin dmvdmvdtFr
HHdtM
t
t
oo
t
to
![Page 24: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/24.jpg)
Conservation of Angular Momentum
If the resultant moment about a fixed point O of all forces acting on a particle is zero during an interval of time, its angular momentum remains constant. In this case, the angular momentum of the particle is said to be conserved. Angular momentum may be conserved about one axis but not about another axis.
210 OOo HHH
This equation expresses the principle of conservation of angular momentum.
OH
![Page 25: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/25.jpg)
PROBLEMS
1. The assembly starts from rest and reaches an angular speed of 150 rev/min under the action of a 20 N force T applied to the string for t seconds. Determine t. Neglect friction and all masses except those of the four 3-kg spheres, which may be treated as particles.
![Page 26: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/26.jpg)
SOLUTION
st
t
HHdtM
sphere
linkspherepulleyv
rmrT
t
tzzz
08.15
4.06021504.0341.020
2
112
z
v
v
v
v
![Page 27: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/27.jpg)
PROBLEMS
2. A pendulum consists of two 3.2 kg concentrated masses positioned as shown on a light but rigid bar. The pendulum is swinging through the vertical position with a clockwise angular velocity =6 rad/s when a 50-g bullet traveling with velocity v=300 m/s in the direction shown strikes the lower mass and becomes embedded in it. Calculate the angular velocity which the pendulum has immediately after impact and find the maximum deflection of the pendulum.
![Page 28: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/28.jpg)
SOLUTIONAngular momentum is conserved during impact;
)(/77.2
2.02.34.02.3050.064.02.362.02.320cos4.0300050.0 2222
ccwsrad
(1)
(2)
21
0
0
, 02112
vmrvmrM
HHHHdtM
O
OOOO
t
O
12
21
´
v1
v1´
v2´
v2
O
![Page 29: Kinetics of Particles Impulse and Momentum](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56815acb550346895dc89c13/html5/thumbnails/29.jpg)
SOLUTION
Energy considerations after impact; 2211 gg VTVT (Datum at O)
o1.52
cos81.94.005.02.3cos81.92.02.30
81.94.005.02.381.92.02.377.22.02.32177.24.02.305.0
21 22
12
21
´
v1
v1´
v2´
v2
O