PH2. Analyzing and Describing Motion

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Last updated 3:35 PM on 8/15/25
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18 Terms

1
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What are the graphs for a ball which is thrown, falls, and is caught

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2
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What is the difference between the graphs for a ball which falls, bounces and is caught?

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3
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How do you find the instantaneous velocity on a curved displacement-time graph?

Draw a tangent at the point and calculate its gradient

<p>Draw a tangent at the point and calculate its gradient</p>
4
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How do you interpret the shape of a displacement-time graph?

- Horizontal line = zero displacement

- Straight line = constant velocity

- Curved line = acceleration

<p>- Horizontal line = zero displacement</p><p>- Straight line = constant velocity</p><p>- Curved line = acceleration</p>
5
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How do you interpret the shape of a velocity-time graph?

- Horizontal line = constant velocity

- Straight line = constant acceleration

- Curved line = changing acceleration

<p>- Horizontal line = constant velocity</p><p>- Straight line = constant acceleration</p><p>- Curved line = changing acceleration</p>
6
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How do you interpret the shape of an acceleration-time graph?

- Horizontal line = constant acceleration

- Straight line = changing acceleration

<p>- Horizontal line = constant acceleration</p><p>- Straight line = changing acceleration</p>
7
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What do the y-intercepts, gradients and areas under graphs represent?

Y-intercept: initial quantity

Gradient of:

- Displacement-time graph is velocity

- Velocity-time graph is acceleration

Area under:

- Velocity-time graph is displacement

- Acceleration-time graph is velocity

<p>Y-intercept: initial quantity</p><p>Gradient of:</p><p>- Displacement-time graph is velocity</p><p>- Velocity-time graph is acceleration</p><p>Area under: </p><p>- Velocity-time graph is displacement</p><p>- Acceleration-time graph is velocity</p>
8
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What are the key features of a bouncing ball's motion at its highest and lowest points under uniform gravity, ignoring air resistance?

Highest Point (A):

Zero velocity

Maximum displacement

Velocity changes from positive to negative

Lowest Point (B):

Constant velocity if no energy loss

Velocity changes from negative to positive

<p>Highest Point (A):</p><p>Zero velocity</p><p>Maximum displacement</p><p>Velocity changes from positive to negative</p><p>Lowest Point (B):</p><p>Constant velocity if no energy loss</p><p>Velocity changes from negative to positive</p>
9
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What general principles describe the motion of a bouncing ball under uniform gravity, ignoring air resistance?

- Constant acceleration downwards due to gravity = 9.8 m s-2

- Positive velocity = upward motion, negative velocity = downward motion

- Deceleration during ascent, acceleration during descent

- Same height after each bounce if air resistance is negligible

<p>- Constant acceleration downwards due to gravity = 9.8 m s-2</p><p>- Positive velocity = upward motion, negative velocity = downward motion</p><p>- Deceleration during ascent, acceleration during descent</p><p>- Same height after each bounce if air resistance is negligible</p>
10
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What is a projectile?

Any object that moves through the air, acted on only by gravity, as drag forces are negligible

<p>Any object that moves through the air, acted on only by gravity, as drag forces are negligible</p>
11
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What are the differences between the horizontal and vertical component in projectile motion?

Horizontal Component:

- Displacement is maximum range at end of motion

- Velocity is constant

- Acceleration is zero

Vertical Component:

- Displacement is maximum height at midpoint (half-time)

- Velocity is zero at maximum height

- Acceleration is g = 9.8m s-2 (positive downward, negative upward)

<p>Horizontal Component:</p><p>- Displacement is maximum range at end of motion</p><p>- Velocity is constant</p><p>- Acceleration is zero</p><p>Vertical Component:</p><p>- Displacement is maximum height at midpoint (half-time)</p><p>- Velocity is zero at maximum height</p><p>- Acceleration is g = 9.8m s-2 (positive downward, negative upward)</p>
12
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What are the horizontal and vertical components of motion for an object projected horizontally with an initial speed U?

Horizontal Motion:

Displacement x = Ut (constant speed)

Velocity vx​ = U (constant)

Vertical Motion:

Displacement y = ½gt² (accelerated by gravity)

Velocity vy​ = −gt (downward acceleration)

13
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Why do two objects—one dropped vertically and the other projected horizontally—hit the ground simultaneously?

- Time of flight depends on the vertical component of motion

- Time is constant as g is constant and height is same

14
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How can we use SUVAT equations to determine the time of flight?

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15
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How can we use SUVAT equations to determine the maximum height?

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16
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How can we use SUVAT equations to determine the horizontal motion?

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17
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How does air resistance affect maximum height and range of a projectile?

- Slows down both components of velocity

- Work done against air resistance reduces kinetic energy

- So maximum height is reached sooner

- Therefore, vertical and horizontal distance decreases

<p>- Slows down both components of velocity</p><p>- Work done against air resistance reduces kinetic energy</p><p>- So maximum height is reached sooner</p><p>- Therefore, vertical and horizontal distance decreases</p>
18
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What would the motion of a projectile look like if gravity were switched off and air resistance were negligible?

Without gravity:

- Projectile travels in a straight line at constant velocity due to initial launch force

- Horizontal displacement is constant x=Utcosθ

- Vertical displacement is constant y=Utsinθ

With gravity:

- Vertical velocity decreases by gt due to gravitational acceleration

- Vertical displacement decreases by ½gt², creating a parabolic trajectory

<p>Without gravity:</p><p>- Projectile travels in a straight line at constant velocity due to initial launch force</p><p>- Horizontal displacement is constant x=Utcosθ</p><p>- Vertical displacement is constant y=Utsinθ</p><p>With gravity:</p><p>- Vertical velocity decreases by gt due to gravitational acceleration</p><p>- Vertical displacement decreases by ½gt², creating a parabolic trajectory</p>

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