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8/18/2019 Dynamics Problem
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Projectile Motion
g~ ax = dvx/dt = 0
ay = dvy/dt = -g
vx = vx,o
vy = vy,o - gt
x = vx,o t + xo
y = yo + vy,o t - gt2
2Friday, November 11, 2011
8/18/2019 Dynamics Problem
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Projectile Motion
g~ ax = dvx/dt = 0
ay = dvy/dt = -g
vx = vx,o
vy = vy,o - gt
x = vx,o t + xo
y = yo + vy,o t - gt2
2Friday, November 11, 2011
8/18/2019 Dynamics Problem
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Projectile Motion
g~ ax = dvx/dt = 0
ay = dvy/dt = -g
vx = vx,o
vy = vy,o - gt
x’
y’
x = vx,o t + xo
y = yo + vy,o t - gt2
2Friday, November 11, 2011
8/18/2019 Dynamics Problem
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Projectile Motion
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8/18/2019 Dynamics Problem
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ExampleGiven: Given vo and #, find the equationthat defines y as a function of x.
Use vx = vo cos # and vy = vo sin #
x = (vo cos #)t or t =x
vo cos !
y = (vo sin #) t – $ g (t)2
Eliminate t :
y = (vo sin !) { } { }2x g x
vo cos ! 2 vo cos ! –
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Example 2
Projectile is fired with vA=150 m/s at point A.
The horizontal distance it travels (R) and thetime in the air.
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Example 2
Establish a fixed x, y coordinate system (in this solution, theorigin of the coordinate system is placed at A). Apply thekinematic relations in x- and y-directions.
Projectile is fired with vA=150 m/s at point A.
The horizontal distance it travels (R) and thetime in the air.
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Example 2
1) Place the coordinate system at point A.
Equation for horizontal motion.
xB = xA + vAx tf where xB = R, xA = 0, vAx = 150 (4/5) m/s
R = 120 tf Time of flight: tf
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Example 2
1) Place the coordinate system at point A.
Equation for horizontal motion.
xB = xA + vAx tf where xB = R, xA = 0, vAx = 150 (4/5) m/s
R = 120 tf
2) Now write a vertical motion equation. Use the distance equation.
yB = yA + vAy tf – 0.5 g tf 2
where yB = – 150, yA = 0, and vAy = 150(3/5) m/s
We get the following equation: –150 = 90 tf + 0.5 (– 9.81) tf 2
Time of flight: tf
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8/18/2019 Dynamics Problem
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Example 2
1) Place the coordinate system at point A.
Equation for horizontal motion.
xB = xA + vAx tf where xB = R, xA = 0, vAx = 150 (4/5) m/s
R = 120 tf
2) Now write a vertical motion equation. Use the distance equation.
yB = yA + vAy tf – 0.5 g tf 2
where yB = – 150, yA = 0, and vAy = 150(3/5) m/s
We get the following equation: –150 = 90 tf + 0.5 (– 9.81) tf 2
Solving for tf first, tf = 19.89 s.
Then, R = 120 tf = 120 (19.89) = 2387 m
Time of flight: tf
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8/18/2019 Dynamics Problem
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Example 3
A skier leaves the ski jump ramp at "A
= 25o and hits the slope at B. Find theSkier’s initial speed, va.
Motion in x-direction:
Using xB = xA + vox(tAB) => (4/5)100 = 0 + vA (cos 25) tAB
=tAB=80
vA
(cos 25°)
88.27
vA
x
y
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Example 3
Motion in y-direction:
Using yB = yA + voy(tAB) – $ g(tAB)2
– 64 = 0 + vA(sin 25°) { }88.27
vA – ! (9.81) { }2
88.27
vA
vA = 19.42 m/s
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Do it in your head1. In a projectile motion problem, what is the maximum number of unknownsthat can be solved?
A) 1 B) 2
C) 3 D) 4
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Do it in your head1. In a projectile motion problem, what is the maximum number of unknownsthat can be solved?
A) 1 B) 2
C) 3 D) 4
2. The time of flight of a projectile, fired over level ground, with initialvelocity Vo at angle #, is equal to?
A) (vo sin ")/g B) (2vo sin ")/g
C) (vo cos ")/g D) (2vo cos ")/g
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Do it in your head
3. A projectile is given an initial velocity
vo at an angle # above the horizontal.
The velocity of the projectile when it
hits the slope is ____________ the
initial velocity vo.
A) less than B) equal to
C) greater than D) None of the above.
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Do it in your head
3. A projectile is given an initial velocity
vo at an angle # above the horizontal.
The velocity of the projectile when it
hits the slope is ____________ the
initial velocity vo.
A) less than B) equal to
C) greater than D) None of the above.
4. A particle has an initial velocity vo at angle " with respect to the horizontal. The
maximum height it can reach is when
A) " = 30° B) " = 45°
C) " = 60° D) " = 90°
Friday November 11 2011