Motion & Kinematics
Describing motion with graphs, SUVAT equations and projectile decomposition.
Spec Points Covered
- I can define and distinguish between displacementThe distance moved in a particular direction from a starting point. A vector quantity. Measured in metres (m)., velocityThe rate of change of displacement. A vector quantity. Measured in m s⁻¹., speed and accelerationThe rate of change of velocityThe rate of change of displacement. A vector quantity. Measured in m s⁻¹.. A vector quantity. Measured in m s⁻². as scalar or vector quantities.
- I can interpret displacementThe distance moved in a particular direction from a starting point. A vector quantity. Measured in metres (m).-time graphs to find velocityThe rate of change of displacement. A vector quantity. Measured in m s⁻¹. from the gradient.
- I can interpret velocity-time graphs to find accelerationThe rate of change of velocity. A vector quantity. Measured in m s⁻². (gradient) and displacementThe distance moved in a particular direction from a starting point. A vector quantity. Measured in metres (m). (area under graph).
- I can interpret accelerationThe rate of change of velocity. A vector quantity. Measured in m s⁻².-time graphs and determine change in velocity from the area under the graph.
- I can select and apply the correct SUVAT equation to problems involving uniform acceleration.
- I can solve multi-stage SUVAT problems where the final velocity of one stage becomes the initial velocity of the next.
- I can describe free fallMotion under gravity alone, with no other forces acting. All objects in free fall near Earth's surface have the same acceleration, g = 9.81 m s⁻². and use g = 9.81 $m s^{-2}$ in calculations, including objects thrown upwards.
- I can resolve projectileAn object moving freely under gravity after being launched. Horizontal and vertical components of motion are independent. motion into independent horizontal and vertical components.
- I can calculate the range, maximum height and time of flight for a projectileAn object moving freely under gravity after being launched. Horizontal and vertical components of motion are independent..
- I can describe experiments to measure the acceleration due to gravity.
Notes
01
Displacement
Displacement
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02
The gradient of a displacement-time graph gives the velocity
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03
The gradient of a velocity-time graph gives the acceleration
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04
The SUVAT equations apply only to motion with constant (uniform) acceleration
$v = u + at$
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05
Free fall
Free fall
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06
Projectile
Projectile
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07
The area under an acceleration-time graph gives the change in velocity
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On Data Sheet
Not on Data Sheet
First SUVAT equation
$$v = u + at$$
- Where:
- $v$ = m \(s^{-1}\)
- $u$ = m \(s^{-1}\)
- $a$ = m \(s^{-2}\)
- $t$ = s
Use when you know u, a, t and want v (or rearrange). No s in this equation.
Second SUVAT equation
$$s = ut + \frac{1}{2}at^{2}$$
- Where:
- $s$ = m
- $u$ = m \(s^{-1}\)
- $a$ = m \(s^{-2}\)
- $t$ = s
Use when you know u, a, t and want s. No v in this equation.
Third SUVAT equation
$$v^{2} = u^{2} + 2as$$
- Where:
- $v$ = m \(s^{-1}\)
- $u$ = m \(s^{-1}\)
- $a$ = m \(s^{-2}\)
- $s$ = m
Use when you know u, a, s and want v, or when time is not given. No t in this equation.
Fourth SUVAT equation
$$s = \frac{(u + v)}{2} \times t$$
- Where:
- $s$ = m
- $u$ = m \(s^{-1}\)
- $v$ = m \(s^{-1}\)
- $t$ = s
Displacement equals average velocity times time. No a in this equation.
Horizontal component of velocity
$$v_{x} = u\cos\theta$$
- Where:
- $v_x$ = m \(s^{-1}\)
- $u$ = m \(s^{-1}\)
Used in projectile problems. The horizontal velocity is constant throughout the flight (no horizontal acceleration).
Vertical component of velocity
$$v_{y} = u\sin\theta$$
- Where:
- $v_y$ = m \(s^{-1}\)
- $u$ = m \(s^{-1}\)
Used in projectile problems. The vertical velocity changes due to gravitational acceleration g.
Average velocity
$$\bar{v} = \frac{\Delta s}{\Delta t}$$
- Where:
- $\bar{v}$ = m \(s^{-1}\)
- $\Delta s$ = m
- $\Delta t$ = s
Average velocity equals total displacement divided by total time.