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Question 12
A particle is moving in simple harmonic motion about the origin, with displacement $x$ metres. The displacement is given by $x = 2 ext{ sin } 3t$, where $t$ is time... show full transcript
Step 1
Answer
To find the distance travelled by the particle when it first returns to the origin, we need to determine the period of the motion. The general formula for simple harmonic motion displacement is given by:
This implies that when the particle returns to the origin, the angle must equal or , for the first complete return.
Given that , we set:
The first return to the origin occurs at:
Thus, the first return occurs at:
At this time, we calculate the total distance travelled. Within half a period:
Step 2
Answer
The particle is at rest when its velocity is zero. The velocity of the particle can be found by differentiating the displacement function:
v(t) = rac{dx}{dt} = 6 ext{ cos }(3t).
Setting this equal to zero to find when the particle is at rest:
6 ext{ cos }(3t) = 0 \ \ ext{ implies } 3t = rac{ ext{π}}{2} \ \ ext{ or } 3t = rac{3 ext{π}}{2}
This gives:
t = rac{ ext{π}}{6} \ \ ext{ or } t = rac{ ext{π}}{2}
The first instance occurs at t = rac{ ext{π}}{6}. Now, substitute back to find the acceleration:
a(t) = rac{d^{2}x}{dt^{2}} = -18 ext{ sin }(3t).
Thus, when t = rac{ ext{π}}{6}:
$$aigg(rac{ ext{π}}{6}igg) = -18 ext{ sin }igg(3 imes rac{ ext{π}}{6}igg) = -18 ext{ sin}igg(rac{ ext{π}}{2}igg) = -18 ext{ (1)} = -18 ext{ m/s}^{2}.$
Step 3
Answer
To find the volume of the solid formed by rotating the region bounded by , the -axis between and x = rac{ ext{π}}{2}, we use the disk method:
$$V = ext{π} ext{ } igg[ ext{ Area integral}igg] = ext{π} ext{ } igg( ext{Area under } y = ext{cos}(4x)igg) = ext{π} ext{ }igg( igg[ rac{1}{2} y^2 igg]_{0}^{rac{ ext{π}}{2}} \ = ext{π} imes igg[ rac{1}{2}( ext{cos}(4 imes rac{ ext{π}}{2}))^2 - rac{1}{2}( ext{cos}(4 imes 0))^2\ = ext{π} imes igg[ rac{1}{2}(0^2) - rac{1}{2}(1^2) \ = -rac{ ext{π}}{2} \ \ V = ext{π} igg[ rac{1}{2}(1 - 0) = rac{ ext{π}}{2} ext{ } ( ext{Final positive volume})igg] = rac{ ext{π}}{2} ext{ m}^{3}.$
Step 4
Answer
The acceleration is given by:
rac{d^{2}x}{dt^{2}} = 2 - rac{x}{2}
To find in terms of , we apply the chain rule:
rac{dv}{dt} = rac{dv}{dx} imes rac{dx}{dt}
This means:
v rac{dv}{dx} = 2 - rac{x}{2}
Integrating:
rac{1}{2} v^2 = 2x - rac{x^2}{4} + C
Given that when :
We can find . Therefore, , giving:
Thus, the complete expression for is:
$$v^2 = 2x - rac{x^2}{4} + 16.$
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