Which of the following functions does NOT describe simple harmonic motion?
- \(x=\cos ^2 t-\sin 2 t\)
- \(x=\sin 4 t+4 \cos 2 t\)
- \(x=2 \sin 3 t-4 \cos 3 t+5\)
- \(x=4 \cos \left(2 t+\dfrac{\pi}{2}\right)+5 \sin \left(2 t-\dfrac{\pi}{4}\right)\)
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Which of the following functions does NOT describe simple harmonic motion?
\(B\)
\(\text{By trial and error}\)
\(\text{Option}\ A:\)
\(x=\cos^2t-\sin\,2t=\dfrac{1}{2}\cos\,2t+\dfrac{1}{2}-\sin\,2t \)
\(\dot x=-\sin\,2t-2\cos\,2t \)
\(\ddot x\) | \(=-2\cos\,2t+4\sin\,2t\) | |
\(=-4\Big(\dfrac{1}{2}\cos\,2t-\sin\,2t\Big) \) | ||
\(=-4\Big(x-\dfrac{1}{2}\Big) \ \ \ \text{(SHM)}\) |
\(\text{Similarly, options}\ C\ \text{and}\ D\ \text{can be differentiated to show} \)
\(\ddot x=-n^2(x-c) \)
\(\text{Consider option}\ B:\)
\(x=\sin\,4t+4\cos\,2t\)
\(\dot x=4\cos\,4t-8\sin\,2t\)
\(\ddot x\) | \(=-16\sin\,4t-16\cos\,2t\) | |
\(= -16(\sin\,4t-\cos\,2t)\ \ \ \ \text{(not SHM)} \) |
\(\Rightarrow B\)
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)`
A particle is moving in simple harmonic motion. The displacement of the particle is `x` and its velocity, `v`, is given by the equation `v^2 = n^2 (2kx - x^2)`, where `n` and `k` are constants.
The particle is initially at `x = k`.
Which function, in terms of time `t`, could represent the motion of the particle?
A. `x = k cos (nt)`
B. `x = k sin (nt) + k`
C. `x = 2k cos (nt) - k`
D. `x = 2k sin (nt) + k`
`B`
`text(Completing the square):`
`v^2 = n^2(2kx-x^2)`
`=n^2(k^2-(x^2-2kx+k^2))`
`=n^2(k^2-(x-k)^2)`
`:.\ text(The centre of motion is)\ \ x = k,\ text(amplitude) = k,`
`⇒ B`
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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What is the earliest time tomorrow at which the tide is increasing at the fastest rate? (2 marks)
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i. | `text(High tide)` | `= 9\ text(m)` |
`text(Low tide)` | `= 1\ text(m)` |
`:. A = (9 – 1)/2 = 4\ text(m)`
`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)` |
ii. `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)`
`text(when)\ \ sin ((4 pi)/25 t) = -1,`
`:. (4 pi)/25 t` | `= (3 pi)/2` |
`= 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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Show that the earliest possible time that the ship can leave the wharf is 4:05 am. (2 marks)
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The ship takes 20 minutes to sail from the wharf to the harbour entrance and it must be out to sea by 7 am. What is the latest time the ship can leave the wharf? (2 marks)
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i. `text(Period)`
`(2pi)/n =` | ` 12.5` |
`12.5n =` | ` 2pi` |
`25n =` | ` 4pi` |
`n =` | ` (4pi)/25` |
`text(Amplitude)`
`a` | `= 1/2(10 − 4)` |
`= 3` |
`=>\ text(Motion centres around)\ \ x = 7\ \ text(with)`
`y = 10\ \ text(when)\ \ t= 0`
`:.\ text(Water depth is given by)`
`y` | `= 7+a cos nt` |
`= 7 + 3 cos\ ((4pit)/(25))\ \ …\ text(as required.)` |
ii. |
`text(Find)\ \ t\ \ text(when)\ \ y = 8.5:`
`8.5` | `= 7 + 3\ cos\ ((4pit)/25)` |
`3\ cos\ ((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(The earliest time the ship can leave)`
`text(is 4:05 am … as required.)`
iii. `text(2 metres above low tide = 6 m)`
`text(Find)\ t\ text(when)\ y = 6:`
`6 = 7 + 3\ cos\ ((4pit)/(25))`
`3\ cos\ ((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(At the harbour entrance, water depth)`
`text(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 moves in a straight line. Its displacement, `x` metres, after `t` seconds is given by
`x = sqrt3\ sin\ 2t − cos\ 2t + 3`.
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i. `text(Show)\ \ ddot x = -4(x − 3)`
`x` | `= sqrt3\ sin\ 2t − cos\ 2t + 3` |
`dot x` | `= 2sqrt3\ cos\ 2t + 2\ sin\ 2t` |
`ddot x` | `= -4sqrt3\ sin\2t + 4\ cos\ 2t` |
`= -4(sqrt3\ sin\ 2t − cos\ 2t)` | |
`= -4(sqrt3\ sin\ 2t − cos\ 2t + 3 − 3)` | |
`= -4(x − 3)\ \ …text(as required)` |
ii. `text(Period)\ = (2pi)/n`
`n^2 = 4 ⇒ n = 2\ \ text{(part (i))}`
`:.\ text(Period)` | `= (2pi)/2` |
`= pi\ \ text(seconds)` |
iii. `text(Write)\ \ dot x = 2sqrt3\ cos\ 2t + 2\ sin\ 2t`
`text(in form)\ \ \ A\ cos\ (2t − α)`
`A(cos\ 2t\ cos\ α + sin\ 2t\ sin\ α)` | `= 2sqrt3\ cos\ 2t + 2\ sin\ 2t` |
`cos\ 2t\ cos\ α + sin\ 2t\ sin\ α` | `= (2sqrt3)/A\ cos\ 2t + 2/A\ sin\ 2t` |
`⇒ cos\ α` | `= (2sqrt3)/A` |
`⇒ sin\ α` | `= 2/A` |
`((2sqrt3)/A)^2 + (2/A)^2` | `= 1` |
`(2sqrt3)^2 + 2^2` | `= A^2` |
`:.A` | `= sqrt16` |
`= 4` |
`:.cos\ α` | `= (2sqrt3)/4 = sqrt3/2` |
`α` | `= pi/6` |
`:. dot x = 4\ cos\ (2t − pi/6)`
(iv) `text(Find)\ \ t\ \ text(when)\ \ dot x = ±2`
`text(If)\ \ dot x = 2`
`4\ cos\ (2t − pi/6)` | `= 2` |
`cos\ (2t − pi/6)` | `= 1/2` |
`2t − pi/6` | `= pi/3, 2pi − pi/3` |
`2t` | `= pi/2, (11pi)/6` |
`t` | `= pi/4, (11pi)/12` |
`text(If)\ \ dot x = -2`
`cos\ (2t − pi/6)` | `= – 1/2` |
`2t − pi/6` | `= (2pi)/3, (4pi)/3` |
`2t` | `= (5pi)/6, (3pi)/2` |
`t` | `= (5pi)/12, (3pi)/4` |
`:.t = pi/4, (5pi)/12, (3pi)/4, (11pi)/12\ \ text(seconds.)`
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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What are the values of `a`, `c` and `n`? (3 marks)
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i. `text(Particle is at rest when)\ v^2 = 0`
`:. x = 3\ \ text(or)\ \ 7`
ii. `text(Maximum speed occurs when)`
`v^2` | `= 11` |
`v` | `= sqrt11\ text(m/s)` |
iii. `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)` |
`= 4n^2` | |
`n^2` | `= 11/4` |
`:.n` | `= sqrt11/2` |
A particle is moving in simple harmonic motion with period 6 and amplitude 5.
Which is a possible expression for the velocity, `v`, of the particle?
`A`
`text(By Elimination:)`
`text(General form is)\ \x = a sin (nt)`
`text(Period) = 6\ text{(given)}`
`=> (2pi)/n` | `= 6` |
`n` | `= pi/3` |
`:.\ text(Cannot be)\ C\ text(or)\ D`
`text(Using)\ \ x = int v\ dt`
`text(Consider answer)\ B`
`x` | `= 5 xx 3/pi sin (pi/3 t) + c` |
`text(Amplitude) = 15/pi` |
`:.\ text(Cannot be)\ B`
`text(Consider answer)\ A`
`x` | `= (5pi)/3 xx 3/pi sin (pi/3 t) + c` |
`= 5 sin (pi/3 t) + c` | |
`:.\ text(Amplitude) = 5` |
`=> A`
The equation of motion for a particle moving in simple harmonic motion is given by
`(d^2x)/(dt^2) = -n^2x`
where `n` is a positive constant, `x` is the displacement of the particle and `t` is time.
where `v = (dx)/(dt)` and `a` is the amplitude of the motion. (3 marks)
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i. | `text(Show)\ \ v^2 = n^2 (a^2\ – x^2)` |
`(d^2x)/(dt^2) = -n^2x`
`d/(dx) (1/2 v^2)` | `= -n^2 x` |
`1/2 v^2` | `= int -n^2x\ dx` |
`= (-n^2 x^2)/2 + c` | |
`v^2` | `= -n^2 x^2 + c` |
`text(When)\ \ v = 0,\ \ x = a`
`0` | `= -n^2a + c` |
`c` | `= n^2 a^2` |
`:.\ v^2` | `= -n^2 x^2 + n^2 a^2` |
`= n^2 (a^2\ – x^2)\ \ text(… as required)` |
ii. | `text(Max speed when)\ \ x = 0` |
`v^2` | `= n^2 (a^2\ – 0)` |
`= n^2 a^2` | |
`:.v_text(max)` | `= na` |
iii. | `(d^2x)/(dt^2)\ \ text(is maximum at limits)\ \ (x = +-a)` |
`(d^2x)/(dt^2)` | `= |n^2 (a)|` |
`= n^2 a` |
iv. | `x` | `= a sin nt` |
`dot x` | `= an cos nt` |
`text(Find)\ \ t\ \ text(when)\ \ dot x = (na)/2`
`(na)/2` | `= an cos nt` |
`cos nt` | `= 1/2` |
`nt` | `= pi/3` |
`:.t` | `= pi/(3n)` |
A particle moves along a straight line. The displacement of the particle from the origin is `x`, and its velocity is `v`. The particle is moving so that `v^2 + 9x^2 = k`, where `k` is a constant.
Show that the particle moves in simple harmonic motion with period `(2pi)/3`. (2 marks)
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`text(Proof)\ \ text{(See Worked Solutions)}`
`v^2 + 9x^2` | `= k` |
`v^2` | `= k\ – 9x^2` |
`1/2 v^2` | `= 1/2k\ – 9/2 x^2` |
`text(For SHM,)\ \ ddot x = -n^2x`
`ddot x` | `= d/(dx) (1/2v^2)` |
`= -9x` | |
`= -3^2 x \ \ \ text(… as required)` |
`text(Period)\ (T)\ text(of SHM) = (2pi)/n`
`text(Here,)\ \ n=3`
`:.T= (2pi)/3\ \ \ text(… as required)`
The equation of motion for a particle undergoing simple harmonic motion is
`(d^2x)/(dt^2) = -n^2 x`,
where `x` is the displacement of the particle from the origin at time `t`, and `n` is a positive constant.
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Find the values of `A` and `B` in the solution `x = A cos nt + B sin nt`. (2 marks)
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i. | `x` | `= A cos nt + B sin nt` |
`(dx)/(dt)` | `= – An sin nt + Bn cos nt` | |
`(d^2x)/(dt^2)` | `= – An^2 cos nt\ – Bn^2 sin nt` | |
`= -n^2 (A cos nt + B sin nt)` | ||
`= -n^2 x\ \ \ text(… as required)` |
ii. `text(At)\ \ t=0, \ x=0, \ v=2n:`
`x` | `= Acosnt + Bsinnt` |
`0` | `= A cos 0 + B sin 0` |
`:.A` | `= 0` |
`text(Using)\ \ (dx)/(dt) = Bn cos nt`
`2n` | `= Bn cos 0` |
`Bn` | `= 2n` |
`:.B` | `= 2` |
iii. `text(Max distance from origin when)\ (dx)/(dt) = 0`
`(dx)/(dt)` | `= 2n cos nt` |
`0` | `= 2n cos nt` |
`cos nt` | `= 0` |
`nt` | `= pi/2,\ (3pi)/2,\ (5pi)/2` |
`t` | `= pi/(2n),\ (3pi)/(2n), …` |
`:.\ text(Particle is first at greatest distance)`
`text(from)\ O\ text(when)\ t = pi/(2n).`
iv. `text(Solution 1)`
`text(Find the distance travelled from)\ \ t=0\ \→\ \ t=(2pi)/n`
`text{(i.e. 1 full period)}`
`text(S)text(ince)\ \ x=2 sin (nt)`
`=> text(Amplitude)=2`
`:.\ text(Distance travelled)=4 xx2=8\ text(units)`
`text(Solution 2)`
`text(At)\ t = 0,\ x = 0`
`text(At)\ t` | `= pi/(2n)` |
`x` | `= 2 sin (n xx pi/(2n)) = 2` |
`text(At)\ t` | `= (3pi)/(2n)\ \ \ text{(i.e. the next time}\ \ (dx)/(dt) = 0 text{)}` |
`x` | `= 2 sin (n xx (3pi)/(2n)) = -2` |
`text(At)\ t` | `= (2pi)/n` |
`x` | `= 2 sin (n xx (2pi)/n) = 0` |
`:.\ text(Total distance travelled)`
`= 2 + 4 + 2` |
`= 8\ \ text(units)` |
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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i. `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)` |
ii. `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.)}` |