© samir n. shoukry, 2004, dynamics mae 242. quiz 2 (5 minutes) a car accelerates according to the...
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![Page 1: © Samir N. Shoukry, 2004, Dynamics MAE 242. Quiz 2 (5 minutes) A car accelerates according to the relation a=0.02s m/s 2. Determine its velocity when](https://reader034.vdocuments.us/reader034/viewer/2022051516/56649cba5503460f94981ab6/html5/thumbnails/1.jpg)
© Samir N. Shoukry, 2004, Dynamics MAE 242
MAE 242: DYNAMICSMAE 242: DYNAMICS
Dr. Samir N. ShoukryDr. Samir N. ShoukryProfessor, MAE & CEEProfessor, MAE & CEE
Class 3Class 3
assistants assistants K. Mc Bride Dhananjy Rao K. Mc Bride Dhananjy Rao
ony Oomen Praveenony Oomen Praveen
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© Samir N. Shoukry, 2004, Dynamics MAE 242
Quiz 2 (5 minutes)Quiz 2 (5 minutes)
A car accelerates according to the relation a=0.02s m/s2. Determine its velocity when s=100 m if s=v=0 when t=0.
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© Samir N. Shoukry, 2004, Dynamics MAE 242
How Position May Be Described?How Position May Be Described?
New York
Morgantown
East
North
West
South
Point of reference that may be placed anywhere …, say Charleston, WV
East
North
West
South
Point of reference that may be placed anywhere …, say Charleston, WV
W
M
N
rM/W
rN/W
East
North
West
South
Point of reference that may be placed anywhere …, say Charleston, WV
East
North
West
South
Point of reference that may be placed anywhere …, say Charleston, WV
W
M
N
rM/W
rN/W
Position is defined relative to a point on which we set a coordinate system Position is defined relative to a point on which we set a coordinate system
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© Samir N. Shoukry, 2004, Dynamics MAE 242
OROR
Position is defined by a vector “r” Position is defined by a vector “r” that originates from a reference pointthat originates from a reference point
Remember: A vector has a length and direction
New York
PathPath
N
EW
S
rM/N
Position VectorPosition Vector
Morganown
New York
Path
Position Vector
New York
Path
Position Vector
rN/M
MorganownN
EW
S
New York
Morgantown
East
North
West
South
New York
Morgantown
East
North
West
South
Morgantown
East
North
West
South
North
West
South
rM/W
rN/W
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© Samir N. Shoukry, 2004, Dynamics MAE 242
X
Y
Z
X
Y
Z
r r = = xx i i + y+ y j j r r = = xx i i + y+ y j j + + z z kk
X
Y
Z
xy
zγ r
β
X
Y
Z
xy
zγ r
β
r
x
y
Y
X
r
x
y
Y
X
Position is defined by the distance from Position is defined by the distance from three perpendicular lines from an origin three perpendicular lines from an origin OO..
Rectangular CoordinatesRectangular Coordinates
222 zyxr
L e n g t h o f r
D i r e c t i o n o f r
z
r
y
r
x
r ||cos,
||cos,
||cos
222 zyxr
L e n g t h o f r
D i r e c t i o n o f r
z
r
y
r
x
r ||cos,
||cos,
||cos
22 yxr
Len g t h o f r
D i r ec t i o n o f r)(tan 1
x
y
22 yxr
Len g t h o f r
D i r ec t i o n o f r)(tan 1
x
y
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© Samir N. Shoukry, 2004, Dynamics MAE 242
Rectangular Coordinates:Rectangular Coordinates:Velocity & AccelerationVelocity & Acceleration
r r = = xx i i + y+ y j j + + z z kk
v v = = vvxx i i + v+ vyy j j + + vvzz kk
a a = = aaxx i i + a+ ayy j j + + aazz kk
ddtv= dr
dt = (xi) (yj) (zk)+ ddt
ddt+ dx
dt i+ didtxd
dt(xi)= = = dxdt i vxi
222zyx vvvv
222zyx aaaa
X
Y
Z
X
Y
Z
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© Samir N. Shoukry, 2004, Dynamics MAE 242
Example: Given , Calculate the magnitude and direction of the velocity and acceleration vectors. Calculate the magnitude of the position vector.
2 32t t r i j k
2 2
22 2 2 1
2 6 , 2 & 6
6(2 ) (6 ) tan
2
x y
drt t v t v t
dt
tv t t v
t
v i j
2 2 1
2 12 , 2 & 12
12(2) (12 ) tan
2
x y
dt a a t
dtt
a t a
va i j
2t
26t
y
v
2 3
2 2 3 2 2
, 3 & 1
( ) (2 ) (1)
x y zr t r t r
r t t
2
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© Samir N. Shoukry, 2004, Dynamics MAE 242
v0xv
0 yv
0v
yv
0x xv v
0y
fy
maxy
R
0x
0x xv v
upxdownx
x
ya gj j
0xa i
Motion of A ProjectileMotion of A Projectile
0
20 0
2 20 0
1
2
2 ( )
v v a t
s s v t a t
v v a s s
0
20 0
2 20 0
:
1
2
2 ( )
y y
y
y y
In y Direction
v v g t
y y v t g t
v v g y y
0
20 0
2 20 0
0
0 0
:
1
2
2 ( )
0
x x x
x x
x x
x
x x
x
In x Direction
v v a t
x x v t a t
v v a x x
If a
v v
x x v t
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© Samir N. Shoukry, 2004, Dynamics MAE 242
MAE 242: DYNAMICSMAE 242: DYNAMICS
Instructor Instructor Dr. Samir N. ShoukryDr. Samir N. ShoukryProfessor, MAE & CEEProfessor, MAE & CEE
assistants assistants Dr. G. William, CEE Dr. G. William, CEE Mr. K. Mc Bride, MAEMr. K. Mc Bride, MAE
Class 4Class 4
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© Samir N. Shoukry, 2004, Dynamics MAE 242
Quiz 3 (5 minutes)Quiz 3 (5 minutes)A particle moves according to the relation r=5t3 i +2t2 j Calculate the magnitude and direction of its acceleration when t =0.5 second.
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© Samir N. Shoukry, 2004, Dynamics MAE 242
Example: A particle accelerates according to the relation: Given the initial conditions at t=0: x, y, z =0 and vx=vy=1 & vz=0, calculate the particle velocity & position.
5yx v t a i j k
22
0 1
2 1
20 0
1
2 2 2
1 , , sinh sinh1
x
x x x xx x
vxx
x
t x
x x
dv dv dv dvdx dxa x v
dt dx dt dt dx dx
vxx dx v dx
dx dxv x v dt t x x t
dt x
0 1 0 0
ln , 1y
y yy y
y
v yt ty t t t
y yy
dv dva v dt
dt v
dvdt t v v e dy e dt y e
v
2 2 3
0 0 0 0
5 5
55 2.5 , 2.5
6
z
zz z
v t z t
z z
dva t dv t dt
dt
dv t dt v t dz t z t
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© Samir N. Shoukry, 2004, Dynamics MAE 242
v0xv
0 yv
0v
yv
0x xv v
0y
fy
maxy
R
0x
0x xv v
upxdownx
x
ya gj j
0xa i
Motion of A ProjectileMotion of A Projectile
0
20 0
2 20 0
1
2
2 ( )
v v a t
s s v t a t
v v a s s
0
20 0
2 20 0
:
1
2
2 ( )
y y
y
y y
In y Direction
v v g t
y y v t g t
v v g y y
0
20 0
2 20 0
0
0 0
:
1
2
2 ( )
0
x x x
x x
x x
x
x x
x
In x Direction
v v a t
x x v t a t
v v a x x
If a
v v
x x v t
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© Samir N. Shoukry, 2004, Dynamics MAE 242
A skier leaves the ramp A at angle with the horizontal. He strikes the ground at point B, Determine his initial speed vA and the time of flight from A to B.
25A
3100( ) 60
5
-64
4100( ) 80
5
cosA Av
sinA Av
20 0
2
Inetial and final positions are given. Thus let us use the
1position relation S=S
2: 80 0 ( cos 25) 0 ..........(1)
1: 64 0 ( sin 25) ...........(2)
2. 1& 2
A
A
A
v t at
In X direction v t
InY direction v t gt
Solve Eq v
19.41 / 4.547m s AND t s
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© Samir N. Shoukry, 2004, Dynamics MAE 242
x
y
15cos 60 7.5 /ft s
15sin 60 12.99 /ft s
20 0
Initial position and velocity are given. The relation between
x and y components of he final position is given.
1Apply in x and y directions.
2: 0 7.5 ............(1)
s s v t at
In x direction x t
In y directi
2
2
1: 0 12.99 ...........(2)
2
: 0.05 ............(3)
& 5.15 1.33
on y t gt
Also we have y x
Solve for x y x ft and y ft
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© Samir N. Shoukry, 2004, Dynamics MAE 242
y5 m
5 5
10 2814
5 5 5
14/
5ft s
20 0
2
, .
1:
228
: 10 0 0.79865
14 1: 0 1.8718 5 1.8718 3.1282
25
: De
Initial velocity and position are given also given x coordinate of the final position
Apply s s v t at
In x direction t t s
In y direction y t gt y m h m
Another Methode
2 2
termine the distance the squirrel drops in time t.
1.5*9.81*.7986 3.1282
2h gt m
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© Samir N. Shoukry, 2004, Dynamics MAE 242
The boy at A attempts to throw a ball over the roof of a barn such that it is launched at an angle of 40 degrees. Determine the speed vA at which he must throw the ball so that it reaches its maximum height at C. Also, find the distance d where the boy must stand so that he can make the throw.
Given: Y0 = 1m, At max. height, vY = 0, Y = 8m and v0x = v0cos400; v0y = v0sin400
(1) X = v0xt; (2) vx = v0x (constant velocity in x-direction);
(3) Y = Y0 1/2gt2 + v0Yt (4) vY = v0Y gt (constant acceleration -g in y-direction)
At the top of the trajectory vy = 0 and from (4) we get: v0y = gt
Substituting the above into (3) we get 7 = ½ g t2 and solving the above to get the time to reach maximum elevation. t = 1.195 seconds Substituting for v0Y at the top of the trajectory, we get v0sin40o = 9.81(1.195)
which is solved for the initial velocity.v0 = 18.24 m/sec
Substituting into (1) we get the total distance X.X = 18.24(cos40)(1.195) = 16.7 mWhich gives d = X 4 = 12.70m
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© Samir N. Shoukry, 2004, Dynamics MAE 242
The ball is thrown from the tower with a velocity of 20 ft/s as shown. Determine the x and y coordinates to where the ball strikes the slope. Also, determine the speed at which the ball hits the ground.Initial Conditions:v0 = 20 ft/s v0x = 20(3/5) = 12 ft/s v0y = 20(4/5) = 16 ft/s
theta = 26.60 , X0 = 0 Y0 = 80 ft
Motion in the x-direction at a constant velocity. (1) vx = v0x = 12 ft/s (2) X = vxt = 12t
Motion in the y-direction at a constant acceleration a = -g. Integrating for velocity(3) vy = v0y - gt = 16 - 32.2(t)
and the y-displacement is obtained by integrating the latter, which givesY = -1/2gt2 + v0yt + Y0
or (4) Y = -16.1t2 +16t + 80The x and y coordinates of the ball when it hits the ground can be written as.(5) x = 20 + Rcos26.6o ; (6) y = Rsin26.6o
Equations (2), (4) (5) and (6) are four equations in four unknowns. They can be solved for t - the time when the ball hits the ground. Thus t = 2.7 sec.Substituting into (2) and (4) provides the x and y coordinates of the ball when it hits the ground. x = 32.4 ft; y = 6.56 ftTo solve for the speed, we substitute t = 2.7s into equation (3) which gives.vx = 12 ft/s and vy = 70.9 ft/s
The total speed is found from v = (vx2 + vy
2)1/2 ; v = 71.9ft/s