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Marina CMI [18]
3 years ago
10

A water balloon launcher uses an elastic band with a spring constant of 115 N/m. To use the launcher, you stretch the band back

with a balloon in it. The water balloons have a mass of 1.3 kg/
a. If you stretch the band by 0.8 m, what elastic force will the band exert?

b. With the band stretched 0.8 m, how much elastic potential energy is stored in the spring?

c. If you release the band, it pushes the balloon forward. What is the kinetic energy of the balloon when it reaches the natural length of the band? Explain how you found the answer.

d. What is the speed of the balloon when it reaches the natural length of the band?
Physics
2 answers:
Lorico [155]3 years ago
7 0

Here elastic balloon launcher will behave like an ideal spring

so here we have

spring constant k = 115 N/m

mass of balloon = 1.3 kg

Part a)

Stretch in the band is given as

x = 0.8 m

now the force on the balloon is given by

F = k x

now from above

F = (115) (0.8) = 92 N

so it will exert 92 N force on it

Part b)

Elastic potential energy is given as

U = \frac{1}{2}kx^2

so here we have

U = \frac{1}{2}(115)(0.8)^2

U = 36.8 J

Part c)

Here in this case we can say that kinetic energy gained by the balloon must be same as the elastic potential energy stored in the rubber because there is no energy loss in this system

So kinetic energy = 36.8 J

Part d)

As we know by the formula of kinetic energy

K = \frac{1}{2}mv^2

36.8 = \frac{1}{2}(1.3)v^2

v = 7.52 m/s

so speed of the balloon will be 7.52 m/s

suter [353]3 years ago
3 0

a) F=kx=92 N

b) PE=1/2*k*x^2=36.8 J

c) Apply law of conservation of energy:

KE=PE=1/2*m*v^2=36.8 J

d) v=\sqrt{\frac{2KE}{m}}=7.52 m/s

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A projectile is fired upward at an angle θ above the horizontal with an initial speed v0. At its maximum height, what are its ve
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Answer:

\vec{v}_{\rm max} = v\cos(\theta)(\^x)\\|\vec{v}_{\rm max}| = v\cos(\theta)\\\vec{a} = \vec{g} = -9.8\^y

Explanation:

The equations of kinematics will be used to solve this question:

y - y_0 = v_{y_0}t + \frac{1}{2}a_yt^2\\v_y^2 = v_{y_0}^2 + 2a_y(y - y_0)\\v_y = v_{y_0} + a_yt

At its maximum height, the projectile has zero velocity in the y-direction. But its velocity in the x-direction is unaffected.

First, let's apply the above equations to the x-direction.

There is no acceleration in the x-direction. So, its velocity in the x-direction is constant during the motion.

v_x = v_{x_0} + a_xt = v_{x_0} + 0\\v_x = v_{x_0} = v\cos(\theta)

Therefore, the velocity vector of the projectile is

v_{max} = v_x = v\cos(\theta)

The speed of the projectile is the same.

The acceleration vector is constant during the motion and equal to the gravitational acceleration, which is -9.8 downwards.

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A flywheel having constant angular acceleration requires 4.00 ss to rotate through 164 radrad . Its angular velocity at the end
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Answer:

\omega '=-13.5rad/s

Explanation:

From the question we are told that:

Time t=4sec

Angular displacement \theta= 161 rad

Final Angular velocity  \omega = 100 rad / s

Let

Angular acceleration \alpha  

Generally the equation for Initial Angular velocity  \omega ' is mathematically given by

-\omega '^2=2 \alpha \theta -\omega^2

\omega '^2= \alpha 328 +11236

Also,Initial Angular velocity  \omega ' is mathematically given by

\omega '=\omega  - \alpha t

Therefore substitution

-\omega '^2=2 \alpha \theta -\omega^2

\omega '=\omega  - \alpha t

(\omega  - \alpha t)^2=2 \alpha \theta -\omega

-16\alpha^2+848\alpha+11236= \alpha 328 -11236

16\alpha^2-520\alpha=0

\alpha=29.875rads/s^2

Substitution in the 2nd equation for Initial Angular velocity  \omega '

\omega '=106-(29.875rads/s^2*4)

\omega '=-13.5rad/s

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