Question #6e509

Question

Question #6e509

2 Answers

Impact of this question

6006 views around the world

You can reuse this answer
Creative Commons License

Answer 1 · 2016-12-24T11:52:52

google

To solve this problem using the knowledge of physics we assume that

the bungee rope behaves as an ideal spring and Hook;s law is obeyed here.
jumper just steps of bridge and falls straight downward.
If the height of the jumper is neglected comparing with the length of the rope, the position of the jumper may be considered as a point.
The loss in gravitational potential energy of the jumper provides the gain in potential energy of the stretched rope at the first lowest position of the jumper, ignoring dissipation of energy during elongation of rope.

Now if the elongation of rope be $x$ $x$ m for first downward trip then gain in PE of the rope will be
$E_{rope} = \frac{1}{2} \times k x^{2}$ $E_"rope"=1/2xxkx^2$

where

$k \to force constant of the rope = 160 N m^{- 1}$ $k->"force constant of the rope "=160Nm^(-1)$

Again the loss PE of jumper

$E_{jumper} = m \times g \times h$ $E_"jumper"=mxxgxxh$

where

$m \to mass of the jumper = 61 k g$ $m->"mass of the jumper"=61kg$

$g \to acceleration due to gravity = 10 m s^{- 2}$ $g->"acceleration due to gravity"=10ms^-2$

$h \to fall of jumper$ $h-> "fall of jumper"$

Here

$h = length of relaxed rope + elongation of rope = (20 + x) m$ $h="length of relaxed rope" + "elongation of rope"=(20+x)m$

So by conservation of energy

$\frac{1}{2} \times k x^{2} = m \times g \times h$ $1/2xxkx^2=mxxgxxh$

$\Rightarrow \frac{1}{2} \times 160 x^{2} = 61 \times 10 \times (20 + x)$ $=>1/2xx160x^2=61xx10xx(20+x)$

$\Rightarrow 8 x^{2} = 61 \times (20 + x)$ $=>8x^2=61xx(20+x)$

$\Rightarrow 8 x^{2} - 61 x - 1220 = 0$ $=>8x^2-61x-1220=0$

$\Rightarrow x = \frac{1}{16} (61 + \sqrt{61^{2} + 4 \times 8 \times 1220}) \approx 16.73 m$ $=>x=1/16(61+sqrt(61^2+4xx8xx1220))~~16.73m$

The jumper jumps from 44m above the water level of the river . If we add the length (20m) of the relaxed rope with the elongation the total elongated length becomes $16.73 + 20 = 36.73 m$ $16.73+20=36.73m$ . This length being less than 44m, the jumper will not hit water..

At this stage the upward force on jumper due to elastic property of the rope $F ↑ = k x = 160 \times 16.73 N$ $Fuarr=kx=160xx16.73N$
and downward gravitational pull $F ↓ = 61 \times 10 N$ $Fdarr=61xx10N$
So net upward pull on the jumper
$F_{net} ↑ = F ↑ - F ↓ = 160 \times 16.73 N - 61 \times 10 N = 2066.8 N$ $F_"net"uarr=Fuarr-Fdarr=160xx16.73N-61xx10N=2066.8N$

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
Let at the final position when oscillation stops the net elongation be $y$ $y$ m

At this stage the gravitational pull is the cause of stretching and by Hook's law we can write

$k \times y = m g$ $kxxy=mg$

$\Rightarrow y = \frac{m g}{k} = \frac{61 \times 10}{160} \approx 3.81 m$ $=>y=(mg)/k=(61xx10)/160~~3.81m$
Adding the length of the relaxed rope with it the lowest final position of the jumper will be $20 + 3.81) = 23.81 m$ $20+3.81)=23.81m$ .

At this position the net force on the jumper will be Zero as he is at rest.

Answer 2 · 2016-12-25T07:09:28

Alternate solution based on solution already posted by @dk_ch.

Explanation:

Following assumptions are made

The bungee rope behaves as an ideal spring and obeys Hook's law.
Jumper just steps off bridge and falls straight downward as shown below. The center of gravity in this position is almost at the level of platform where the jumper stands.
![http://www.ukbungee.co.uk](https://useruploads.socratic.org/ay43gASdRxquYDQPNLR9_jumptype_24_0_large.jpg)
The other end of rope is tied at the center of gravity of the jumper. The picture of jumper at the time of reaching the lowest point is as shown below. As such the effective height of platform is taken as if the thickness of jumper is neglected as compared to the length of the rope.
![dangerous-business.com]()

The loss in gravitational potential energy of the jumper gets converted into kinetic energy of the jumper till relaxed length of rope is reached. Thereafter further loss of potential energy and kinetic energy is used to stretch the rope.

Taking downward direction as positive $x$ $x$ -axis and origin at the point where rope has no slack.

Potential energy stored in the stretched rope

$P E_{rope} = \frac{1}{2} k x^{2}$ $PE_"rope"=1/2kx^2$
where $k$ $k$ is spring constant of the rope $= 160 N m^{- 1}$ $=160Nm^(-1)$
$x$ $x$ is elongation of the rope.

Also the loss of PE of jumper at the lowest point

$P E_{jumper} = m g h$ $PE_"jumper"=mgh$
where $m$ $m$ is mass of the jumper.
$g$ $g$ acceleration due to gravity $= 9.81 m s^{- 2}$ $=9.81ms^-2$
$h$ $h$ is maximum fall of jumper $="length of relaxed rope"+x_max$

$:. h=(20+x_max)m$
By conservation of energy we get
$1/2kx_max^2=mg(20+x_max)$

Inserting given values we get
$1/2 xx160x_max^2=61xx9.81xx(20+x_max)$
$=>80x_max^2=11968.2+598.41x_max$
$=>80x_max^2-598.41x_max-11968.2$

Plotting this equation using the graphic tool and taking only the positive root as length can not be negative we get

my comp

$=>x_max=16.53m$

It is given that the jumper jumps from bridge $44m$ above the river. We see that lowest point is at a distance of $h=20+16.53=36.53m$ from the bridge. This length is less than $44m$ . Therefore, the jumper will not get wet.

At this point only two force are acting on the jumper.
A. the upward force on jumper which can be found using Spring equation for force

$F=-kx$
$F=-160xx16.53N$ ,
$-ve$ sign shows that force is in the upward direction.

B. Downward force as weight $=mg=61xx9.81N$

Net force on the jumper is sum of both forces $=-160xx16.53+61xx9.81$
$=-2046.4N$ , rounded to one decimal place.

Science

Math

Humanities

... and beyond

Question #6e509

2 Answers

Explanation:

Related questions

Impact of this question