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Figure 12-57 shows an approximate plot of stress versus strain for a spider-web thread, out to the point of breaking at a strain of 0.200. The vertical axis scale is set by values a=0.12 GN/m2, b=0.30 GN/m2, and c=0.80 GN/m2 . Assume that the thread has an initial length of 0.80 cm, an initial cross-sectional area of 8.0x10-12 m2, and (during stretching) a constant volume. Assume also that when the single thread snares a flying insect, the insect’s kinetic energy is transferred to the stretching of the thread. (a) How much kinetic energy would put the thread on the verge of breaking? What is the kinetic energy of (b) a fruit fly of mass 6.00 mg and speed 1.70 m/s and (c) a bumble bee of mass 0.388 g and speed 0.420 m/s ? Would (d) the fruit fly and (e) the bumble bee break the thread?

Short Answer

Expert verified
  1. Kinetic energy that would put the thread on the verge of breaking is 3.03×10-5J
  2. The kinetic energy of fruit fly of mass 6.00 mg and speed 1.70 m/s is 8.67×10-6J
  3. The kinetic energy of a bumble bee of mass 0.388 g and speed 0.420 m/s is3.42×10-5J
  4. Fruit fly will not be able to brake the thread
  5. The bumble bee will be able to break the thread

Step by step solution

01

Determine the given quantities

The vertical axis scale is set by valuesis as follows:

a=0.12 GN/m2

b=0.30 GN/m2

c= 0.80 GN/m2

Initial length of thread is 0.80 cm and initial cross-sectional area of 8.0×10-12m2

02

Determine the concept of work done and kinetic energy

From the area of the graph, find the work done. find the kinetic energy of the given insects and objects using the formula in terms of mass and velocity. Comparing these two values, we can decide whether thread would break or not.

Consider the formula for the work done:

W=∫Fdx ….. (i)

Here, W is work done, F is force, and dx is change in displacement.

Solve for the kinetic energy as:

K=12mv2 ….. (ii)

Here, K is kinetic energy, m is mass and v is speed.

03

(a) Determine Kinetic energy that would put the thread on the verge of breaking.

Consider the formula for the work done:

W=∫Fdx

Consider the formula for the force as:

F=stress×area

Consider the case of very small length is:

dx=strain×length

Consider the formula for the work done as:

W=∫stress×A×strain×L=AL∫stress×strain=crosssectionalareaofthread×lengthofthread×areaunderthecurveoflength

The area under the curve is obtained as:

Areaunderthecurveofgraph=12as1+12a+bs2-s1+12b+cs3-s2=12as2+bs3-s1+cs3-s2=120.12×109N/m21.4+0.30×109N/m21.0+0.80×109N/m20.60=4.74×108N/m2

Therefore, the kinetic energy can be calculated as,

K=8.0×10-12N/m28.0×10-3m4.74×108N/m2=3.03×10-5J

Kinetic energy that would put the thread on the verge of breaking is 3.03×10-5J

04

(b) Determine the kinetic energy of fruit fly of mass   and speed  

Consider the expression for the kinetic energy as:

Kf=12mfvf2=12×6.00×10-6kg1.70m/s22=8.67×10-6J

The kinetic energy of fruit fly of mass 6.00 mg and speed 1.70 m/s2 is 8.67×10-6J

05

(c) Determine the kinetic energy of a bumble bee of mass   and speed  

Consider the formula for the kinetic energy as:

Kb=12mbvb2

Substitute the values and solve as:

Kb=12×3.99×10-4kg0.420m/s22=3.42×10-5J

The kinetic energy of a bumble bee of mass 0.388 g and speed 0.420 m/s2 is 3.42×10-5J.

06

Explanation of part d

From the explanation it is clear that:

Fruit fly will not be able to break the thread, because Kf<W .

07

Explanation of part e

From the explanation it is clear that:

The bumble bee will be able to break the thread, because Kb>W .

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Most popular questions from this chapter

The system in Fig. 12-38 is in equilibrium. A concrete block of mass225kghangs from the end of the uniform strut of mass45.0kg. A cable runs from the ground, over the top of the strut, and down to the block, holding the block in place. For anglesϕ=30.0°andθ=45.0°, find (a) the tension Tin the cable and the (b) horizontal and (c) vertical components of the force on the strut from the hinge.

In Fig. 12-69, a package of mass mhangs from a short cord that is tied to the wall via cord 1 and to the ceiling via cord 2. Cord 1 is at angleϕ=40°with the horizontal; cord 2 is at angleθ. (a) For what value of θis the tension in cord 2 minimized? (b) In terms of mg, what is the minimum tension in cord 2

A physical therapist gone wild has constructed the (stationary) assembly of massless pulleys and cords seen in Fig. 12-24. One long cord wraps around all the pulleys, and shorter cords suspend pulleys from the ceiling or weights from the pulleys. Except for one, the weights (in newtons) are indicated.

(a) What is that last weight? (Hint:When a cord loops halfway around a pulley as here, it pulls on the pulley with a net force that is twice the tension in the cord.)

(b) What is the tension in the short cord labeled T?

Question: Figure 12-29 shows a diver of weight 580 N standing at the end of a diving board with a length of L =4.5 mand negligible v mass. The board is fixed to two pedestals (supports) that are separated by distance d = 1 .5 m. Of the forces acting on the board, what are the (a) magnitude and (b) direction (up or down) of the force from the left pedestal and the (c) magnitude and (d) direction (up or down) of the force from the right pedestal? (e) Which pedestal (left or right) is being stretched, and (f) which pedestal is being compressed?

The force F→ in Fig. 12-70 keeps the 6.40 k²µ block and the pulleys in equilibrium. The pulleys have negligible mass and friction. Calculate the tension Tin the upper cable. (Hint:When a cable wraps halfway around a pulley as here, the magnitude of its net force on the pulley is twice the tension in the cable.)

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