Title: Plane Curvilinear Motion
1Plane Curvilinear Motion
2Lecture Goals
- Rectangular Coordinates
- Polar Coordinates
- Normal and Tangential Coordinates
3Rectangular Coordinates
Using 2-D rectangular coordinates, the location,
velocity and acceleration can be represented in
Cartesian form of equation. A change in the
vector, displacement is represented as
4Rectangular Coordinates
The velocity component is represented by The
acceleration by
5Example Problem Rectangular systems
A projectile is fired with an initial velocity
of 800 ft/s at a target B located 2000 ft above
the gun A and at a horizontal distance of 12000
ft. Neglect air resistance, determine the value
of the firing angle a.
6Example Problem Rectangular systems
Break the problem into horizontal and vertical
components. The horizontal velocity is
7Example Problem Rectangular systems
The distance traveled will be 12000 ft. So the
time can be found
8Example Problem Rectangular systems
The vertical components of the equation are
9Example Problem Rectangular systems
Substitute for the time and the location of 2000
ft.
Use the substitute that 1/cos2 a sec2 a 1
tan2 a
10Example Problem Rectangular systems
Rearrange the equation
Solve the quadratic tan a 0.565 and tan a
2.75
11Example Problem Rectangular systems
The solution will be a 29.5o and a 70.0o,
either angle will reach the target
12Class Problem Rectangular systems
A player throws a ball with an initial velocity
v0 of 50 ft/s from a point A located 5 ft above
the floor. Knowing that the ceiling of the
gymnasium is 20 ft high, determine the highest
point B at which the ball can strike the wall 60
ft. away.
13Polar Coordinates
Using 2-D rectangular coordinates, the location,
velocity and acceleration can be related to point
with angle and radius. So the particle location
is given as where, O is the location of the
reference point.
14Polar Coordinates
The velocity component is represented by The
vector displacement can be represented as
15Polar Coordinates
The vector component can be represented
as Back substitute
16Polar Coordinates
The velocity component are written as
Alternative representation of the vectors is
using Cartesian coordinates.
17Polar Coordinates
Take the derivative of the vector components with
respect to q
18Polar Coordinates
The acceleration can be written as
19Polar Coordinates
The rearrange the acceleration if r is
constant
20Example Problem Polar systems
The rotation of 3 ft arm OA about O is defined by
the relation q 0.15t2, where q is expressed in
radians and t in seconds. Block B slides along
the arm in such a way that it distance from O is
r 3 0.4 t2, where r is expressed in ft and t
in seconds. Determine the total velocity and
total acceleration of block B after the arm OA
has rotated 30o
21Example Problem Polar systems
Find out when q 30o occurs
22Example Problem Polar systems
Take the time derivatives of r and q
23Example Problem Polar systems
The velocity components are
24Example Problem Polar systems
The velocity components are The v 1.744
ft/s and b 31.0o
25Example Problem Polar systems
The acceleration components are
26Example Problem Polar systems
The velocity components are
27Example Problem Polar systems
The velocity components are The a 1.770
ft/s2 and g 42.5o
28Class Problem
Determine the velocity of the rocket and
acceleration in terms of
29Tangential Coordinates
Using 2-D rectangular coordinates, the location,
velocity and acceleration can be related to the
path of the particle radius. So the particle
path is s(t), the velocity along the path is
tangent to the instant in time.
30Tangential Coordinates
The acceleration component is represented by
The vector can be represented as
31Polar Coordinates
The vector component can be represented as
32Tangential Coordinates
The acceleration component is represented by
33Polar Coordinates
The rearrange the acceleration if r is
constant
34Homework (Due 4/14/03)
Problems
13-103, 13-109,13-106, 13-112ab (not c)