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Graphical Model of Motion. We will combine our Kinematics Equations with our Graphical Relationships to describe One Dimensional motion! We will be looking.

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Presentation on theme: "Graphical Model of Motion. We will combine our Kinematics Equations with our Graphical Relationships to describe One Dimensional motion! We will be looking."— Presentation transcript:

1 Graphical Model of Motion

2 We will combine our Kinematics Equations with our Graphical Relationships to describe One Dimensional motion! We will be looking at seven graphs!

3 Graphs for Constant Velocity Velocity = constant (Acceleration = 0) v = d/t From the equation v = d/t, make a data table with t, d, v, a. – Time is the independent variable

4 Displacement vs Time Graph for Constant Velocity d vs t is linear – y = mx +b Slope (m) from a d vs t graph is always, Velocity! Since graph is linear, slope (m) is Constant! Therefore: Velocity is Constant!!

5 Displacement vs Time Graph for Constant Velocity The y-intercept (b) = Where you are starting from when t=0! Graphing a Complete trip! – Every graph tells a story! – Time keeps going even when you are not! – We can find the Instantaneous Velocity, Average Speed and Average Velocity.

6 Velocity vs Time Graph for Constant Velocity Since the Velocity is constant, the graph is a horizontal line (Constant Relationship) Slope of a velocity vs time graph is always acceleration! Since the slope of a horizontal line is zero and the slope is the acceleration, Therefore: acceleration = 0!

7 Velocity vs Time Graph for Constant Velocity We can find the displacement from a velocity vs time graph by finding the Area Under the Curve! d = Area under the Curve Area will be a rectangle: – A = l x w = displacement

8 Acceleration vs Time Graph for Constant Velocity Since the acceleration = zero the graph is a horizontal line on the x-axis (a = 0). We cannot find anything from this graph!

9 Uniform Acceleration Graphs Acceleration (a) is constant. Make a Data Table with your Kinematics Equations Looking a four graphs.

10 Velocity vs Time Graph for Uniform Acceleration v vs t is linear – y = mx +b Slope (m) from a v vs t graph is always, Acceleration! Since graph is linear, slope (m) is Constant! Therefore: Acceleration is Constant!!

11 Velocity vs Time Graph for Uniform Acceleration The y-intercept (b) = Your Initial Velocity (v i ). The speed you are starting with when t=0! y = mx + b becomes; v = at + v i similar to v f = v i + at

12 Velocity vs Time Graph for Uniform Acceleration We can find the displacement from a velocity vs time graph by finding the Area Under the Curve! d = Area under the Curve Area will now be a triangle: – A = ½ b x h = displacement – Similar to d = ½ (v f +v i )t (starting from rest)

13 Displacement vs Time Graph for Uniform Acceleration d vs t is parabolic – y = kx 2 Slope (m) from a d vs t graph is Velocity! Since graph is parabolic, the slope is Not Constant! Therefore: Velocity is Not Constant! (The object is accelerating)

14 Displacement vs Time Graph for Uniform Acceleration d vs t is parabolic, y = kx 2 Unit for the constant (k) is m/s 2 k = half the acceleration (1/2 a) y = kx 2 becomes; d = ½ at 2 Similar to d = v i t + ½ at 2 (Starting from rest v i = 0)

15 Displacement vs Time Squared Graph for Uniform Acceleration Squaring the Time will straighten out the parabola and make the graph linear. d vs t 2 is linear – y = mx +b Slope (m) from a d vs t 2 graph is half the acceleration (1/2 a) Since graph is linear, slope (m) is Constant! (The acceleration is still constant)

16 Acceleration vs Time Graph for Uniform Acceleration Since the Acceleration is constant, the graph is a horizontal line (Constant Relationship) We can find the change in velocity (  v) from an acceleration vs time graph by finding the Area Under the Curve!  v = Area under the Curve Area will be a rectangle: – A = l x w = change in velocity (  v)

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