73. ferris wheel a ferris wheel 50 ft in diameter makes one revolution every 40 sec. if the center of the…

73. ferris wheel a ferris wheel 50 ft in diameter makes one revolution every 40 sec. if the center of the wheel is 30 ft above the ground, how long after reaching the low point is a rider 50 ft above the ground?

73. ferris wheel a ferris wheel 50 ft in diameter makes one revolution every 40 sec. if the center of the wheel is 30 ft above the ground, how long after reaching the low point is a rider 50 ft above the ground?

Answer

Explanation:

Step1: Model the Ferris wheel motion

The height ( h(t) ) of a rider on a Ferris wheel can be modeled using a sinusoidal function. The general form for the height as a function of time ( t ) (after reaching the low point) is ( h(t)=A\sin(\omega t)+k ), where ( A ) is the amplitude, ( \omega ) is the angular frequency, and ( k ) is the vertical shift (center height).

  • The diameter of the Ferris wheel is 50 ft, so the radius ( A = \frac{50}{2}=25 ) ft.
  • The center of the wheel is 30 ft above the ground, so ( k = 30 ) ft.
  • The period ( T = 40 ) sec. The angular frequency ( \omega=\frac{2\pi}{T}=\frac{2\pi}{40}=\frac{\pi}{20} ) rad/sec.

Since we start at the low point, the sine function is shifted. At ( t = 0 ), ( h(0)=30 - 25 = 5 ) ft (low point). The correct model considering the start at low point is ( h(t)=25\sin\left(\frac{\pi}{20}t-\frac{\pi}{2}\right)+30 ) (because the sine function starts at 0, to start at -1 (low point), we shift it by ( -\frac{\pi}{2} )) or we can also use a cosine function with a phase shift. Alternatively, we can use ( h(t)=25\cos\left(\frac{\pi}{20}t+\pi\right)+30 ), but it's easier to adjust the sine function. Let's use the sine function with a phase shift such that at ( t = 0 ), ( h(0) = 5 ).

We want to find ( t ) when ( h(t)=50 ) ft.

So, set up the equation: [ 50=25\sin\left(\frac{\pi}{20}t-\frac{\pi}{2}\right)+30 ]

Step2: Solve for ( t )

First, subtract 30 from both sides: [ 50 - 30=25\sin\left(\frac{\pi}{20}t-\frac{\pi}{2}\right) ] [ 20 = 25\sin\left(\frac{\pi}{20}t-\frac{\pi}{2}\right) ] Divide both sides by 25: [ \sin\left(\frac{\pi}{20}t-\frac{\pi}{2}\right)=\frac{20}{25}=\frac{4}{5} ]

Recall that ( \sin\left(x-\frac{\pi}{2}\right)=-\cos(x) ), so: [ -\cos\left(\frac{\pi}{20}t\right)=\frac{4}{5} ] [ \cos\left(\frac{\pi}{20}t\right)=-\frac{4}{5} ]

We know that ( \cos(\theta)=-\frac{4}{5} ), so ( \theta=\arccos\left(-\frac{4}{5}\right) ). Also, ( \cos(\theta)=\cos(2\pi - \theta) ), but we are looking for the time when the rider is 50 ft above the ground. Let's solve ( \frac{\pi}{20}t=\arccos\left(-\frac{4}{5}\right) )

First, calculate ( \arccos\left(-\frac{4}{5}\right) ). We know that ( \cos(\alpha)=-\frac{4}{5} ), so ( \alpha=\pi-\arccos\left(\frac{4}{5}\right) ). Let's compute ( \arccos\left(\frac{4}{5}\right)\approx0.6435 ) radians, so ( \alpha=\pi - 0.6435\approx2.4981 ) radians.

Now, solve for ( t ): [ t=\frac{2.4981\times20}{\pi}\approx\frac{49.962}{\pi}\approx16. \text{Wait, let's check the equation again.}

Wait, the correct model: when at the low point (( t = 0 )), the height is ( 30 - 25=5 ) ft. The height function can also be written as ( h(t)=25\cos\left(\frac{\pi}{20}t+\pi\right)+30 ), because ( \cos(\pi)= - 1 ), so at ( t = 0 ), ( h(0)=25\times(-1)+30 = 5 ) ft (correct). Let's use this cosine model.

Set ( h(t)=50 ): [ 50=25\cos\left(\frac{\pi}{20}t+\pi\right)+30 ] Subtract 30: [ 20 = 25\cos\left(\frac{\pi}{20}t+\pi\right) ] Divide by 25: [ \cos\left(\frac{\pi}{20}t+\pi\right)=\frac{4}{5} ] Using the identity ( \cos(A + \pi)=-\cos(A) ), so: [ -\cos\left(\frac{\pi}{20}t\right)=\frac{4}{5} ] [ \cos\left(\frac{\pi}{20}t\right)=-\frac{4}{5} ] Which is the same as before. Now, the general solution for ( \cos(x)=-\frac{4}{5} ) is ( x = 2n\pi\pm\arccos\left(-\frac{4}{5}\right) ), ( n\in\mathbb{Z} ). We are looking for the first positive ( t ) (after reaching the low point) when ( h(t)=50 ).

We know that ( \arccos\left(-\frac{4}{5}\right)=\pi-\arccos\left(\frac{4}{5}\right)\approx3.1416 - 0.6435 = 2.4981 ) radians.

So, ( \frac{\pi}{20}t=2.4981 ) (taking the principal solution in ( [0, 2\pi] ) for the first time when the height is 50, since after the low point, the rider moves up, reaches the center at ( t = 10 ) sec (quarter period), top at ( t = 20 ) sec (half period, height ( 30 + 25 = 55 ) ft), wait, wait, the top height is ( 30 + 25 = 55 ) ft? Wait, the problem says "how long after reaching the low point is a rider 50 ft above the ground". Wait, the center is 30 ft, radius 25 ft, so top height is ( 30 + 25 = 55 ) ft, so 50 ft is below the top.

Wait, maybe my model is wrong. Let's re - model the height. Let's take the low point as ( t = 0 ), so the height function can be written as ( h(t)=30 - 25\cos\left(\frac{\pi}{20}t\right) ). Because at ( t = 0 ), ( \cos(0)=1 ), so ( h(0)=30 - 25 = 5 ) ft (low point). At ( t = 20 ) sec (half period), ( \cos(\pi)=-1 ), so ( h(20)=30 + 25 = 55 ) ft (top point). At ( t = 10 ) sec (quarter period), ( \cos\left(\frac{\pi}{2}\right)=0 ), so ( h(10)=30 ) ft (center height). This model makes more sense. Let's use this: ( h(t)=30 - 25\cos\left(\frac{\pi}{20}t\right) )

Now, set ( h(t)=50 ): [ 50=30 - 25\cos\left(\frac{\pi}{20}t\right) ] Subtract 30 from both sides: [ 20=-25\cos\left(\frac{\pi}{20}t\right) ] Divide both sides by - 25: [ \cos\left(\frac{\pi}{20}t\right)=-\frac{20}{25}=-\frac{4}{5} ] Now, we need to solve for ( t ): [ \frac{\pi}{20}t=\arccos\left(-\frac{4}{5}\right) ] We know that ( \arccos\left(-\frac{4}{5}\right)=\pi-\arccos\left(\frac{4}{5}\right) ). Let's calculate ( \arccos\left(\frac{4}{5}\right)\approx0.6435 ) radians, so ( \arccos\left(-\frac{4}{5}\right)\approx3.1416 - 0.6435 = 2.4981 ) radians.

Then, [ t=\frac{2.4981\times20}{\pi}\approx\frac{49.962}{3.1416}\approx16 \text{ sec? Wait, no, let's check with the correct model.}

Wait, ( h(t)=30 - 25\cos\left(\frac{\pi}{20}t\right) ). Let's plug ( t = \frac{40}{3}\approx13.33 ) sec? Wait, let's solve the equation ( 30 - 25\cos\left(\frac{\pi}{20}t\right)=50 ) [ -25\cos\left(\frac{\pi}{20}t\right)=20 ] [ \cos\left(\frac{\pi}{20}t\right)=-\frac{4}{5} ] The general solution for ( \cos(x)=-\frac{4}{5} ) is ( x = 2n\pi\pm\arccos\left(-\frac{4}{5}\right) ), ( n\in\mathbb{Z} ). We want the smallest positive ( t ), so we take ( x=\arccos\left(-\frac{4}{5}\right) ) (since ( \cos(x) ) is negative in the second quadrant, and we are moving from the low point ( ( t = 0 ), ( x = 0 ), ( \cos(0)=1 )) up, so as ( t ) increases, ( \frac{\pi}{20}t ) increases, and ( \cos\left(\frac{\pi}{20}t\right) ) decreases from 1 to - 1. We want to find when ( \cos\left(\frac{\pi}{20}t\right)=-\frac{4}{5} )

We know that ( \cos(\theta)=-\frac{4}{5} ), so ( \theta=\arccos\left(-\frac{4}{5}\right)\approx2.498 ) radians. Then, [ t=\frac{2.498\times20}{\pi}\approx\frac{49.96}{3.1416}\approx16 \text{ sec? Wait, but the top is at } t = 20 \text{ sec with height } 55 \text{ ft. So 50 ft is between } t = 10 \text{ sec (center, 30 ft)} \text{ and } t = 20 \text{ sec (top, 55 ft)? Wait, no, from low point (t = 0, 5 ft) to center (t = 10, 30 ft) to top (t = 20, 55 ft). So 50 ft is between t = 10 and t = 20.

Wait, let's recalculate ( \arccos\left(-\frac{4}{5}\right) ). Using a calculator, ( \arccos\left(-\frac{4}{5}\right)\approx2.498 ) radians. Then ( t=\frac{2.498\times20}{\pi}\approx16 ) sec? Wait, ( \frac{\pi}{20}t = 2.498 ), so ( t=\frac{2.498\times20}{\pi}\approx16 ). But let's check the height at t = 16:

( h(16)=30 - 25\cos\left(\frac{\pi}{20}\times16\right)=30 - 25\cos\left(\frac{4\pi}{5}\right) )

( \cos\left(\frac{4\pi}{5}\right)=\cos(144^{\circ})=-\cos(36^{\circ})\approx - 0.8090 )

So ( h(16)=30 - 25\times(-0.8090)=30 + 20.225 = 50.225\approx50 ) ft. So that's correct.

Step3: Verify the solution

We used the height function ( h(t)=30 - 25\cos\left(\frac{\pi}{20}t\right) ), which is valid because:

  • At ( t = 0 ), ( h(0)=30 - 25\cos(0)=30 - 25 = 5 ) ft (low point).
  • The period ( T=\frac{2\pi}{\omega}=\frac{2\pi}{\frac{\pi}{20}} = 40 ) sec, which matches the given period.

When we solved ( 30 - 25\cos\left(\frac{\pi}{20}t\right)=50 ), we got ( \cos\left(\frac{\pi}{20}t\right)=-\frac{4}{5} ), and then found ( t\approx\frac{\arccos\left(-\frac{4}{5}\right)\times20}{\pi}\approx16 ) sec (more precisely, let's calculate ( \arccos\left(-\frac{4}{5}\right) ) in radians:

( \arccos\left(-\frac{4}{5}\right)=\pi-\arccos\left(\frac{4}{5}\right) )

( \arccos\left(\frac{4}{5}\right)\approx0.6435 ) radians, so ( \arccos\left(-\frac{4}{5}\right)\approx3.1416 - 0.6435 = 2.4981 ) radians.

Then ( t=\frac{2.4981\times20}{\pi}\approx\frac{49.962}{3.1416}\approx16. ) (actually, ( \frac{49.962}{3.1416}\approx16 ) when rounded to a reasonable decimal place. But let's do it more accurately.

( \frac{2.4981\times20}{3.1415926536}\approx\frac{49.962}{3.1415926536}\approx16. ) (exactly, let's see, ( \frac{4}{5}) of the way from 10 to 20? Wait, no, the angle ( \frac{\pi}{20}t ) when ( t = 16 ) is ( \frac{4\pi}{5}=144^{\circ} ), which is in the second quadrant, and ( \cos(144^{\circ})=-\cos(36^{\circ})\approx - 0.8 ), and ( - 25\times(-0.8)=20 ), so ( 30 + 20 = 50 ), which is correct.

Answer:

(\approx 16.7) seconds (more precisely, (\frac{20}{\pi}\arccos\left(-\frac{4}{5}\right)\approx\frac{20}{\pi}(2.4981)\approx16.7) seconds) or approximately 17 seconds. But from the calculation above, when we did the exact substitution, we saw that ( t\approx16 ) seconds (with a small error due to rounding). The exact value is ( t=\frac{20}{\pi}\arccos\left(-\frac{4}{5}\right) \approx 16.7 ) seconds.