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`
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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a. `text{Proof (See Worked Solutions.)}`
b. `pi\ text(seconds)`
c. `dot x = 4\ cos\ (2t − pi/6)`
d. `t = pi/4, (5pi)/12, (3pi)/4, (11pi)/12\ text(seconds.)`
a. `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)` |
b. `text(Period)\ = (2pi)/n`
`n^2 = 4 ⇒ n = 2\ \ text{(part (i))}`
| `:.\ text(Period)` | `= (2pi)/2` |
| `= pi\ \ text(seconds)` |
c. `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)`
d. `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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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 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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a. `text(Proof)\ \ text{(See Worked Solutions)}`
b. `na`
c. `n^2 a`
d. `pi/(3n)`
| a. | `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)` |
| b. | `text(Max speed when)\ \ x = 0` |
| `v^2` | `= n^2 (a^2\ – 0)` |
| `= n^2 a^2` | |
| `:.v_text(max)` | `= na` |
| c. | `(d^2x)/(dt^2)\ \ text(is maximum at limits)\ \ (x = +-a)` |
| `(d^2x)/(dt^2)` | `= |n^2 (a)|` |
| `= n^2 a` |
| d. | `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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a. `text(Proof)\ \ text{(See Worked Solutions)}`
b. `A = 0,\ B = 2`
c. `t = pi/(2n)`
d. `text(8 units)`
| a. | `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)` |
b. `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` |
c. `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 from)\ O\ text(when)\ t = pi/(2n).`
d. `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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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.)}` |