A particle in simple harmonic motion has speed \(v \ \text{ms}^{-1}\), given by \(v^2=-x^2+2 x+8\) where \(x\) is the displacement from the origin in metres.
What is the amplitude of the motion?
- 1 m
- 3 m
- 6 m
- 9 m
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A particle in simple harmonic motion has speed \(v \ \text{ms}^{-1}\), given by \(v^2=-x^2+2 x+8\) where \(x\) is the displacement from the origin in metres.
What is the amplitude of the motion?
\(B\)
\(\text{Using} \ \ v^2=n^2\left(a^2-(x-c)^2\right):\)
| \(v^2\) | \(=-x^2+2 x+8\) |
| \(=9-\left(x^2-2 x+1\right)\) | |
| \(=9-(x-1)^2\) |
\(\therefore a^2 = 9\ \ \Rightarrow\ \ a=3\)
\(\Rightarrow B\)
A particle moves in simple harmonic motion described by the equation
\( \ddot{x}=-9(x-4) . \)
Find the period and the central point of motion. (2 marks)
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\(\text{Period}\ = \dfrac{2 \pi}{3} \)
\(\text{Centre of Motion:}\ x=4 \)
\( \ddot{x}=-9(x-4) \)
\( \Rightarrow\ n=3,\ \ c=4 \)
\(\text{Period}\ = \dfrac{2 \pi}{3} \)
\(\text{Centre of Motion:}\ x=4 \)
A particle is undergoing simple harmonic motion with period `frac{pi}{3}`. The central point of motion of the particle is at `x = sqrt(3)`. When `t = 0` the particle has its maximum displacement of `2 sqrt(3)` from the central point of motion.
Find an equation for the displacement, `x`, of the particle in terms of `t`. (3 marks)
`x = 2 sqrt(3) cos (6t) + sqrt(3)`
| `text{Period}` | `= frac{pi}{3}` |
| `frac{2 pi}{n}` | `= frac{pi}{3}` |
| `n` | `= 6` |
`text{Amplitude} = 2 sqrt(3)`
`text{Centre of motion} = sqrt(3)`
`text{S} text{ince maximum displacement at}\ \ t = 0:`
`x = 2 sqrt(3) cos (6t) + sqrt(3)`
The tide can be modelled using simple harmonic motion.
At a particular location, the high tide is 9 metres and the low tide is 1 metre.
At this location the tide completes 2 full periods every 25 hours.
Let `t` be the time in hours after the first high tide today.
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a. `text(See Worked Solutions)`
b. `11:22:30\ text(am)`
a. `text(High tide = 9m, Low tide = 1 m)`
`A = (9-1)/2 = 4\ text(m)`
`\text{Since}\ \ T = 25/2:`
`(2 pi)/n= 25/2\ \ =>\ \ n=(4 pi)/25`
`text(Centre of motion) = 5`
`text(S) text(ince high tide occurs at)\ \ t = 0,`
`x= 5 + 4 cos (nt)= 5 + 4 cos ((4 pi)/25 t)`
b. `x = 5 + 4 cos ((4 pi)/25 t)`
| `(dx)/(dt)` | `= -4 · (4 pi)/25 *sin ((4 pi)/25 t)` |
| `= -(16 pi)/25 *sin ((4 pi)/25 t)` |
`text(Tide increases at maximum rate when)\ \ sin ((4 pi)/25 t) = -1:`
`(4 pi)/25 t= (3 pi)/2\ \ =>\ \ t=75/8= 9\ text(hours 22.5 minutes)`
`:.\ text(Earliest time is)\ 11:22:30\ text(am)`
The rise and fall of the tide is assumed to be simple harmonic, with the time between successive high tides being 12.5 hours. A ship is to sail from a wharf to the harbour entrance and then out to sea. On the morning the ship is to sail, high tide at the wharf occurs at 2 am. The water depths at the wharf at high tide and low tide are 10 metres and 4 metres respectively.
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a. `text{Proof (See Worked Solutions)}`
b. `text{Proof (See Worked Solutions)}`
c. `4:28\ text(am)`
a. `text(Period)`
`(2pi)/n=12.5\ \ =>\ \ n=(4pi)/25`
`text{Amplitude}\ (a) = 1/2(10-4)= 3`
`y=10\ \ \text{at}\ \ t=0\ \text{(low tide):`
`=>\ text(Motion centres around)\ \ x = 7`
`:. y= 7+acos(nt)= 7 + 3 cos((4pit)/(25))\ \ …\ text(as required.)`
`text(Find)\ t\ text(when)\ \ y = 8.5:`
| `7 + 3cos((4pit)/25)` | `= 8.5` |
| `3cos((4pit)/25)` | `= 1.5` |
| `cos((4pit)/25)` | `= 1/2` |
| `(4pit)/25` | `=pi/3` |
| `t` | `=(25pi)/(3 xx 4pi)=2 1/12= 2\ text(hrs 5 mins)` |
`:.\ text(Earliest time a ship can leave is 4:05 am … as required.)`
c. `text(2 metres above low tide = 6 m)`
`text(Find)\ t\ text(when)\ y = 6:`
| `7 + 3cos((4pit)/(25))` | `=6` |
| `3cos((4pit)/(25))` | `= -1` |
| `cos((4pit)/(25))` | `= -1/3` |
| `(4pit)/25` | `= 1.9106…` |
| `:.t` | `= (25 xx 1.9106…)/(4pi)= 3.801…= 3\ text{hr 48 min (nearest min)}` |
`text(Harbour entrance depth of 6 m occurs when)\ \ t = 2\ text(hr 48 min.)`
`:.\ text(Given 20 mins sailing time, the latest the ship can)`
`text(leave the wharf is at)\ \ t = 2\ text(hr 28 min, or 4:28 am.)`
A particle is moving along the `x`-axis in simple harmonic motion. The displacement of the particle is `x` metres and its velocity is `v` ms`\ ^(–1)`. The parabola below shows `v^2` as a function of `x`.
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a. `3\ text(or)\ 7`
b. `V = sqrt11\ text(m/s)`
c. `a = 2, c = 5, n = (sqrt11)/2`
a. `text(Particle is at rest when)\ v^2 = 0`
`:. x = 3\ \ text(or)\ \ 7`
b. `text(Maximum speed occurs when)`
| `v^2` | `= 11` |
| `v` | `= sqrt11\ text(m/s)` |
c. `v^2 = n^2(a^2-(x-c)^2)`
`text(Amplitude) = 2\ \ =>\ \ a = 2`
`text(Centre of motion when)\ x = 5\ \ =>\ \ c = 5`
`text(S)text(ince)\ \ v^2 = 11\ \ text(when)\ \ x = 5`
| `11` | `= n^2(2^2-(5-5)^2)` |
| `11` | `= 4n^2` |
| `n^2` | `= 11/4` |
| `:.n` | `= sqrt11/2` |
A particle is moving in a straight line according to the equation
`x = 5 + 6 cos 2t + 8 sin 2t`,
where `x` is the displacement in metres and `t` is the time in seconds.
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a. `text(Proof)\ \ text{(See Worked Solutions)}`
b. `1.5\ text(seconds)\ text{(1 d.p.)}`
a. `text(Prove)\ ddot x = -n^2(x\ – c)`
| `x` | `= 5 + 6 cos 2t + 8 sin 2t` |
| `dot x` | `= -12 sin 2t + 16 cos 2t` |
| `ddot x` | `= – 24 cos 2t\ – 32 sin 2t` |
| `= -4 (6 cos 2t + 8 sin 2t)` | |
| `= -2^2 (5 + 6 cos 2t + 8 sin 2t\ – 5)` | |
| `= -2^2 (x\ – 5)\ \ \ text(… as required)` |
b. `text(Find)\ \ t\ \ text(when)\ \ x=0\ \ text(for 1st time:)`
| `5 + 6 cos 2t + 8 sin 2t` | `= 0` |
| `6 cos 2t + 8 sin 2t` | `= -5` |
| `6/10 cos 2t+ 8/10 sin 2t` | `=-1/2` |
| `=>cos theta=6/10\ \ text(and)\ \ sin theta=8/10` | |
| `cos 2t cos theta+sin 2t sin theta` | `=- 1/2` |
| `cos(2t\ – theta)` | `= – 1/2` |
`text(S)text(ince)\ \ cos\ pi/3 = 1/2\ \ text(and)\ cos\ text(is negative)`
`text(in the 2nd and 3rd quadrants,)`
`=>2t\ – theta = pi\ – pi/3,\ pi + pi/3`
`text(We need the 1st time)\ \ x = 0`
| `text(S)text(ince)\ \ cos theta` | `= 6/10` |
| `theta` | `= 0.9273…` |
| `:.\ 2t\ – 0.9273…` | `= (2pi)/3` |
| `2t` | `= (2pi)/3 + 0.9273…` |
| `t` | `= 1/2 ((2pi)/3 + 0.9273…)` |
| `= 1.5108…` | |
| `= 1.5\ text(seconds)\ text{(1 d.p.)}` |