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torisob [31]
3 years ago
4

To penetrate armor, a projectile's point concentrated force in a small area, creating a stress large enough that the armor fails

. A species of jellyfish launches a pointed needle that can penetrate the hard shell of a crustacean. The rapid deceleration on impact creates a 32 μN force on the tip, which has a very small 15 nm radius.How does this compare to the ultimate stress of steel?
Physics
1 answer:
saveliy_v [14]3 years ago
3 0

We know that the equiation of Stress is,

\sigma = \frac{F}{A}

Where

F= Force

A= Area

Here the Force is basically,

F=32\mu N= 32*10^{-6}N

And we know as well, that

A= \pi r^2 =  \pi 15*10^{-9}m

So,

\sigma = \frac{32.10^{-6}}{\pi (15*10^{-9})^2}

\sigma = 4.53*10^{10}N/m^2

For this question, we know that the ultimate stress of steel is 1020Mpa

\sigma_{steel}=1020Mpa=1020*10^6Pa

So the ratio,

R=\frac{\sigma}{\sigma_{steel}}=\frac{4.53*10^{10}}{0.084*10^{10}}

R= 44.38

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7 0
3 years ago
QUESTION 20
Kobotan [32]

a) 0.4 m/s^2

We can find the acceleration of the box by using the suvat equation:

s=ut+\frac{1}{2}at^2

where

s is the distance travelled

u is the initial velocity

t is the time

a is the acceleration

For the box in the problem,

s = 16 m

t = 9 s

u = 0 (it starts from rest)

Solving for a, we find the acceleration:

a=\frac{2s}{t^2}=\frac{2(16)}{9^2}=0.4 m/s^2

C) Tension force in the chain: 446 N

In order to find the normal force, we have to write the equation of the forces along the vertical direction.

We have 3 forces acting along this direction on the box:

- The normal force, N, upward

- The force of gravity, mg, downward (where m= mass of the box and g = acceleration of gravity)

- The vertical component of the tension of in the chain, T sin \theta, upward

So the equation of the forces along the vertical direction is

N+Tsin \theta - mg = 0 (1)

Along the horizontal direction, instead, we have the following equation:

T cos \theta - \mu N = ma (2)

where

T cos \theta is the horizontal component of the tension in the chain

\mu N is the frictional force

a is the acceleration

From (1) we write

N=mg-T sin \theta

And substituting into (2),

T cos \theta - \mu (mg-T sin \theta) = ma\\T cos \theta - \mu mg + \mu T sin \theta = ma\\T = \frac{ma+\mu mg}{cos \theta + \mu sin \theta}

And substituting:

m = 100 kg

\theta=25^{\circ}

\mu=0.46

a=0.4 m/s^2

g=9.8 m/s^2

We find the tension in the chain:

T = \frac{(100)(0.4)+(0.46)(100)(9.8)}{cos 25 + 0.46 sin 25}=446 N

B) Normal force: 792 N

We can now find the normal force by using again equation (1):

N+Tsin \theta - mg = 0

And substituting:

T = 446 N

m = 100 kg

\theta=25^{\circ}

g=9.8 m/s^2

We find:

N=mg-T sin \theta=(100)(9.8)-(446)(sin 25)=792 N

3 0
3 years ago
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