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mariarad [96]
3 years ago
15

You are trying to get to class on time using the UCF Shuttle. You are later than usual getting to the stop and see the shuttle p

ulling away from the stop while you are still 3.9 m behind the bus stop. In 40.9 m you will reach a barrier and you must catch the shuttle before that point. The shuttle has a constant acceleration of 4.5 m/s2. What is the minimum velocity you have to run at to catch the bus before it reaches the barrier
Physics
1 answer:
aivan3 [116]3 years ago
4 0

Answer:

20.1 m/s

Explanation:

Since You are later than usual getting to the stop and see the shuttle pulling away from the stop while you are still 3.9 m behind the bus stop. And In 40.9 m you will reach a barrier and you must catch the shuttle before that point.

Given that the shuttle has a constant acceleration of 4.5 m/s2. 

The total distance to cover is:

Total distance = 40.9 + 3.9 = 44.8 m

Assuming you are starting from rest. Then initial velocity U = 0

Using the 3rd equation of motion to calculate the minimum velocity.

V^2 = U^2 + 2as

V^2 = 0 + 2 × 4.5 × 44.8

V^2 = 403.2

V = sqrt (403.2)

V = 20.1 m/s

Therefore, the minimum velocity you have to run at to catch the bus before it reaches the barrier is 20.1 m/s

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Answer:

An electric motor converts electrical energy into mechanical energy. The process is as follows:

D. When current flows through the motor, it powers electromagnets that are attracted and repelled by the poles of permanent magnets in the motor. The movement of the electromagnets turns a rod in the motor, which makes the mechanical energy available.

6 0
3 years ago
A 0.017 g coin sliding to the right at 0.255 m/s makes an elastic head-on collision with a 0.040 g coin that is initially at res
zysi [14]

Answer:

\approx 0.154\:\mathrm{m/s}

Explanation:

In all collisions, whether elastic or inelastic, momentum must be conserved. Therefore, we can write an equation using the conservation of momentum:

m_{c1}v_{c1,i}+m_{c2}v_{c2,i}=m_{c1}v_{c1,f}+m_{c2}v_{c2,f}

Solving for v_{2c,f}:

0.000017\cdot 0.255+0.000040\cdot0=0.000017\cdot (-0.108)+0.000040\cdot v_{c2,f},\\v_{c2,f}\approx \boxed{0.154\:\mathrm{m/s}}

*Notes:

-It's important to convert g to kg, as kg is the SI unit of mass

-The negative sign in a velocity measure represents direction

-Since the velocity we solved for is positive, it implies that the direction is to the right

5 0
3 years ago
•. Parking orbit is -
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Answer:

Parking orbit is -

a. The path along which a plane travels

b. Orbit of a polar satellite

c. Orbit of geostationary satellite

d. Orbit of the earth.

Explanation:

7 0
3 years ago
Read 2 more answers
(II) A 0.72-m-diameter solid sphere can be rotated about an axis through its center by a torque of 10.8 m • N which accelerates
kozerog [31]

Answer:

m = 23.3 kg

Explanation:

As we know that it will have constant torque on it

so the acceleration of the ball will be constant so here we can say that we can use kinematics equation

\theta = \omega_i t + \frac{1}{2}\alpha t^2

160(2\pi) = 0 + \frac{1}{2}\alpha (15^2)

320 \pi = 112.5 \alpha

so we have

\alpha = \frac{320\pi}{112.5}

\alpha = 8.94 rad/s^2

now we know that

\tau = I \alpha

10.8 = I(8.94)

I = 1.21 kg m^2

so we know that

I = \frac{2}{5}mR^2

here we know that

diameter = 0.72 m

so radius (R) = 0.36 m

\frac{2}{5}m(0.36^2) = 1.21

m = 23.3 kg

8 0
3 years ago
While taking a shower, you notice that the shower head is made up of 44 small round openings, each with a radius of 2.00 mm. You
Julli [10]

To solve the problem it is necessary to apply the concepts related to the calculation of discharge flow, Bernoulli equations and energy conservation in incompressible fluids.

PART A) For the calculation of the velocity we define the area and the flow, thus

A = \pi r^2

A = pi (2*10^{-3})^2

A = 12.56*10^{-6}m^2

At the same time the rate of flow would be

Q = \frac{1L}{2s}

Q = 0.5L/s = 0.5*10^{-3}m^3/s

By definition the discharge is expressed as

Q = NAv

Where,

A= Area

v = velocity

N = Number of exits

Q = NAv

Re-arrange to find v,

v = \frac{Q}{NA}

v = \frac{0.5*10^{-3}}{44*12.56*10^{-6}}

v = 0.9047m/s

PART B) From the continuity equations formulated by Bernoulli we can calculate the speed of water in the pipe

P_1 + \frac{1}{2}\rho v_1^2+\rho gh_1 = P_2 +\frac{1}{2}\rho v^2_2 +\rho g h_2

Replacing with our values we have that

1.5*10^5 + \frac{1}{2}(1000) v_1^2+(1000)(9.8)(0) = 10^5 +\frac{1}{2}(1000)(0.9047)^2 +(1000)(9.8)(5.7)

v_1^2 = 10^5 +\frac{1}{2}(1000)(0.9047)^2 +(1000)(9.8)(5.7)-1.5*10^5 - \frac{1}{2}(1000)

v_1 = \sqrt{10^5 +\frac{1}{2}(1000)(0.9047)^2 +(1000)(9.8)(5.7)-1.5*10^5 - \frac{1}{2}(1000)}

v_1 = 3.54097m/s

PART C) Assuming that water is an incomprehensible fluid we have to,

Q_{pipe} = Q_{shower}

v_{pipe}A_{pipe}=v_{shower}A_{shower}

3.54097*A_{pipe}=0.9047*12.56*10^{-6}

A_{pipe} = \frac{0.9047*12.56*10^{-6}}{3.54097}

A_{pipe = 3.209*10^{-6}m^2

3 0
4 years ago
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