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Using Calculus in 1D Simplified Revision Notes

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2.2.1 Using Calculus in 1D

Variable Acceleration

The motion of an object can be modelled by using formulas given in terms of time.

e.g., x=t36t+8x = t^3 - 6t + 8 can be used to model the position x of a particle at time t seconds.

Sketching this curve

  • Roots: t = 4, 2 (from calculator)
  • Intercept: 8
  • Minimum point: t = 3, x = -1 Min point: t=3x=336(3)+8=1\text{Min point: } t = 3 \Rightarrow x = 3^3 - 6(3) + 8 = -1
image

In this situation, the turning point of the particle is the point at which the particle has no speed, i.e., the particle is stationary.

Terminology

  • Displacement: How far a particle is from the origin where negative and positive directions matter.
  • Distance: How far something has travelled relative to an origin.

image

In this situation, the person walks a distance of 7 m, displacing himself 7 m from the origin.

In this example, he walks a distance of 6m, displacing himself 6m from the origin.

Definitions:

infoNote
  • Velocity: Rate of change of displacement (direction matters).
  • Speed: Rate of change of distance (direction doesn't matter).

Differentiation and Integration:

infoNote
ddts=displacementdt\frac{d}{dt} s = \text{displacement} \quad \Rightarrow \quad \int dtv=dsdt=velocitydtv = \frac{ds}{dt} = \text{velocity} \quad \Rightarrow \quad \int dta=dvdt=d2sdt2=accelerationa = \frac{dv}{dt} = \frac{d^2 s}{dt^2} = \text{acceleration}

Velocity-Time Graph (vt)(v-t):

  • Max Velocity
  • Acceleration: accel=ΔvΔt=dvdt\text{accel} = \frac{\Delta v}{\Delta t} = \frac{dv}{dt}
  • Stationary when v = 0 image

Displacement-Time Graph (sts-t):

  • Max displacement (when v = 0)
  • ΔsoverΔt\Delta s over \Delta t
  • v=ΔsΔt=dsdtv = \frac{\Delta s}{\Delta t} = \frac{ds}{dt}
  • At origin image

infoNote

Example: A particle is travelling with the trajectory s=t2+6t4s = t^2 + 6t - 4.

  1. Find its velocity in terms of t and therefore its minimum displacement.
  2. Comment on the acceleration of the particle. a) The velocity vv is given by:
v=dsdt=2t+6v = \frac{ds}{dt} = 2t + 6

At minimum displacement, ds/dt = 0:

2t+6=02t=6t=3 When t=3:2t + 6 = 0 \quad \Rightarrow \quad 2t = -6 \quad \Rightarrow \quad t = -3\ When\ t = -3:s=(3)2+6(3)4=9184=13 ms = (-3)^2 + 6(-3) - 4 = 9 - 18 - 4 = \mathbf{-13 \text{ m}}

(Negative time tt indicates the time before the reference point.)

b) The acceleration a is given by:

a=dvdt=2a = \frac{dv}{dt} = 2

Acceleration is positive and constant, which means the particle will get faster and faster.


infoNote

A particle PP moves in a straight line such that its distance, s meters, from a fixed point OO at time tt is given by:

s=0.4t30.3t21.8t+5,0t3s = 0.4t^3 - 0.3t^2 - 1.8t + 5, \quad 0 \leq t \leq 3

The diagram shows the displacement-time graph of the motion of PP.

a) Determine the time at which PP is moving with minimum velocity.

b) Find the displacement of PP from OO at this time.

c) Find the velocity of PP at this time.

Solution:

a)

s=0.4t30.3t21.8t+5s = 0.4t^3 - 0.3t^2 - 1.8t + 5 v=dsdt=1.2t20.6t1.8v = \frac{ds}{dt} = 1.2t^2 - 0.6t - 1.8 dvdt=2.4t0.6=0\frac{dv}{dt} = 2.4t - 0.6 = 0

Velocity is at maximum or minimum when dv/dt = 0:

2.4t0.6=0t=0.62.4=14 seconds2.4t - 0.6 = 0 \Rightarrow t = \frac{0.6}{2.4} = \mathbf{\frac{1}{4} \text{ seconds}}

b) Let t=0.25t = 0.25:

s=0.4(0.25)30.3(0.25)21.8(0.25)+5=4.5375 ms = 0.4(0.25)^3 - 0.3(0.25)^2 - 1.8(0.25) + 5 = \mathbf{4.5375 \text{ m}}

c) Let t=0.25t = 0.25:

v=1.2(0.25)20.6(0.25)1.8=1.2375 ms1v = 1.2(0.25)^2 - 0.6(0.25) - 1.8 = \mathbf{-1.2375 \text{ ms}^{-1}}

Integration in Variable Acceleration Problems

infoNote

Example: Given that V=4t2t3V = 4t^2 - t^3 and that initially a particle is at the origin, find the total displacement in the first 8 seconds of motion of the particle.

Method 1: Differential Equations

dsdt=4t2t3s=(4t2t3)dt\frac{ds}{dt} = 4t^2 - t^3 \Rightarrow s = \int (4t^2 - t^3) \, dts=4t33t44+cs = \frac{4t^3}{3} - \frac{t^4}{4} + c

Using the initial condition:

Let t=0,s=00=4(0)33044+cc=0\text{Let } t = 0, \, s = 0 \Rightarrow 0 = \frac{4(0)^3}{3} - \frac{0^4}{4} + c \Rightarrow c = 0s=4t33t44\therefore s = \frac{4t^3}{3} - \frac{t^4}{4}

For t=8t = 8:

s=4(8)33844=10243ms = \frac{4(8)^3}{3} - \frac{8^4}{4} = \mathbf{-\frac{1024}{3} \, \text{m}}

Method 2: Integration with Limits

s=08(4t2t3)dts = \int_0^8 (4t^2 - t^3) \, dt

Using the calculator:

08(4x2x3)dx=10243\int_0^8 (4x^2 - x^3) \, dx = \mathbf{-\frac{1024}{3}}

infoNote

Q4 (Jan 2011, Q6) The velocity vms1v \, \text{ms}^{-1} of a particle at time t is given by v=t29v = t^2 - 9. The particle travels in a straight line and passes through a fixed point OO when t=2.(t,s)=(2,0)t = 2. (t, s) = (2, 0)

  1. (i) Find the displacement of the particle from O when t=0.t = 0.
  2. (ii) Calculate the distance the particle travels from its position at t=0t = 0 until it changes its direction of motion.
  3. (iii) Calculate the distance of the particle from O when the acceleration of the particle is 10ms2.10 \, \text{ms}^{-2}.

Solution:

  1. (i)
v=t29c=(t29)dt=13t39t+cv = t^2 - 9 \Rightarrow \text{c} = \int (t^2 - 9) \, dt = \frac{1}{3} t^3 - 9t + c

Let (t,s)=(2,0)(t, s) = (2, 0):

0=13(2)39(2)+cc=9(2)13(2)30 = \frac{1}{3} (2)^3 - 9(2) + c \Rightarrow c = 9(2) - \frac{1}{3} (2)^3 s=13t39t+463s = \frac{1}{3} t^3 - 9t + \frac{46}{3}

When t=0t = 0, s=463s = \mathbf{\frac{46}{3}}.


  1. (ii) Note: When a particle changes direction, v = 0.
v=t29=0t2=9t=3v = t^2 - 9 = 0 \Rightarrow t^2 = 9 \Rightarrow t = 3

For t=3t = 3, s=13(3)39(3)+463=83s = \frac{1}{3}(3)^3 - 9(3) + \frac{46}{3} = -\frac{8}{3}.

t=0s=463t = 0 \Rightarrow s = \frac{46}{3}

Distance from start:

463(83)=18\frac{46}{3} - \left(-\frac{8}{3}\right) = \mathbf{18} image
  1. (iii)
dvdt=2t=10t=5\frac{dv}{dt} = 2t = 10 \Rightarrow t = 5

When t=5t = 5:

s=13(5)39(5)+463=12s = \frac{1}{3} (5)^3 - 9(5) + \frac{46}{3} = \mathbf{12}
infoNote

Q5 (Jun 2014, Q3) A particle PP travels in a straight line. The velocity of PP at time tt seconds after it passes through a fixed point AA is given by (0.6t2+3)ms1(0.6t^2 + 3) \, \text{ms}^{-1}. Find

  1. (i) the velocity of P when it passes through A.
  2. (ii) the displacement of P from A when t = 1.5.
  3. (iii) the velocity of P when it has acceleration 6ms26 \, \text{ms}^{-2}.

Solution:

  1. (i)
v=0.6t2+3att=0,v=3ms1v = 0.6t^2 + 3 \Rightarrow \text{at} \, t = 0, \, v = \mathbf{3 \, \text{ms}^{-1}}
  1. (ii)
s=(0.6t2+3)dts=0.6t33+3t+cs = \int (0.6t^2 + 3) \, dt \Rightarrow s = \frac{0.6t^3}{3} + 3t + c

At t=0,s=0t = 0, \, s = 0:

0=0+cc=00 = 0 + c \Rightarrow c = 0 S=0.2t3+3tatt=1.5,s=0.2(1.5)3+3(1.5)=5.175mS = 0.2t^3 + 3t \Rightarrow \text{at} \, t = 1.5, \, s = 0.2(1.5)^3 + 3(1.5) = \mathbf{5.175 \, \text{m}}
  1. (iii)
dvdt=1.2t=6t=5\frac{dv}{dt} = 1.2t = 6 \Rightarrow t = 5 v=0.6(5)2+3=18ms1v = 0.6(5)^2 + 3 = \mathbf{18 \, \text{ms}^{-1}}
infoNote

Q8. (OCR 4761, Jan 2008, Q5)

A toy car is moving along the straight line Ox, where O is the origin. The time t is in seconds. At time t=0t = 0 the car is at A, 3 m from O as shown in Fig. 5. The velocity of the car, vms1v \, \text{ms}^{-1}, is given by

v=2+12t3t2v = 2 + 12t - 3t^2

Calculate the distance of the car from O when its acceleration is zero.


Solution:

  1. Integrate velocity to find displacement:
s=(2+12t3t2)dt=2t+6t2t3+cs = \int (2 + 12t - 3t^2) \, dt = 2t + 6t^2 - t^3 + c
  1. At t=0,s=3t = 0, s = 3:
3=2(0)+6(0)2(0)3+c3 = 2(0) + 6(0)^2 - (0)^3 + c c=3\Rightarrow c = 3

So,

s=2t+6t2t3+3s = 2t + 6t^2 - t^3 + 3
  1. Find acceleration by differentiating velocity:
a=dvdt=126ta = \frac{dv}{dt} = 12 - 6t
  1. Set acceleration to zero and solve for tt:
126t=012=6tt=212 - 6t = 0 \Rightarrow 12 = 6t \Rightarrow t = 2
  1. Substitute t=2t = 2 into the displacement equation:
s=2(2)+6(2)2(2)3+3=23ms = 2(2) + 6(2)^2 - (2)^3 + 3 = \mathbf{23 \, \text{m}}
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