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vova2212 [387]
3 years ago
13

Please help me and get 15 points and Brainlessly!!!!!!!

Physics
1 answer:
aleksandrvk [35]3 years ago
4 0

Answer:

A

Explanation:

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True or false? The plates keep moving and are still moving today.
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Why was the idea of plate tectonics difficult for many scientists to accept for many years after it was first introduced?
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3 years ago
A heat engine accepts 200,000 Btu of heat from a source at 1500 R and rejects 100,000 Btu of heat to a sink at 600 R. Calculate
diamong [38]

To solve the problem it is necessary to apply the concepts related to the conservation of energy through the heat transferred and the work done, as well as through the calculation of entropy due to heat and temperatra.

By definition we know that the change in entropy is given by

\Delta S = \frac{Q}{T}

Where,

Q = Heat transfer

T = Temperature

On the other hand we know that by conserving energy the work done in a system is equal to the change in heat transferred, that is

W = Q_{source}-Q_{sink}

According to the data given we have to,

Q_{source} = 200000Btu

T_{source} = 1500R

Q_{sink} = 100000Btu

T_{sink} = 600R

PART A) The total change in entropy, would be given by the changes that exist in the source and sink, that is

\Delta S_{sink} = \frac{Q_{sink}}{T_{sink}}

\Delta S_{sink} = \frac{100000}{600}

\Delta S_{sink} = 166.67Btu/R

On the other hand,

\Delta S_{source} = \frac{Q_{source}}{T_{source}}

\Delta S_{source} = \frac{-200000}{1500}

\Delta S_{source} = -133.33Btu/R

The total change of entropy would be,

S = \Delta S_{source}+\Delta S_{sink}

S = -133.33+166.67

S = 33.34Btu/R

Since S\neq   0 the heat engine is not reversible.

PART B)

Work done by heat engine is given by

W=Q_{source}-Q_{sink}

W = 200000-100000

W = 100000 Btu

Therefore the work in the system is 100000Btu

4 0
3 years ago
A potter's wheel is spinning with an initial angular velocity of 11 rad/s . It rotates through an angle of 80.0 rad in the proce
Grace [21]
  • The angular acceleration of the wheel approximately <u>-0.76 rad/s² or proportionally as deceleration approximately 0.76 rad/s</u>.
  • It need approximately <u>14.474 s</u> to come to rest.

<h2>Introduction</h2>

Hi ! I will help you to discuss about Proportionally Changes in Circular Motion. The analogy of proportionally changes in circular motion is same as the analogy of proportionally changes in direct motion. Here you will hear again the terms acceleration and change in speed, only expressed in the form of a certain angle coverage. Before that, in circular motion, it is necessary to know the following conditions:

  • 1 rotation = 2π rad
  • 1 rps = 2π rad/s
  • 1 rpm = \sf{\frac{1}{60} \: rps} = \sf{\frac{1}{30}\pi \: rad/s}

<h2>Formula Used</h2>

The following equations apply to proportionally changes circular motion:

<h3>Relationship between Angular Acceleration and Change of Angular Velocity </h3>

\boxed{\sf{\bold{\omega_t = \omega_0 + \alpha \times t}}}

With the following conditions:

  • \sf{\omega_t} = final angular velocity  (rad/s)
  • \sf{\omega_0} =  initial angular velocity (rad/s)
  • \sf{\alpha} = angular acceleration (rad/s²)
  • t = interval of the time (s)
<h3>Relationship between Angular Acceleration and Change of \sf{\theta} (Angle of Rotation) </h3>

\boxed{\sf{\bold{\theta = \omega_0 \times t + \frac{1}{2} \times \alpha \times t^2}}}

Or

\boxed{\sf{\bold{(\omega_t)^2= (\omega_0)^2 + 2 \times \alpha \times \theta}}}

With the following condition :

  • \sf{\theta} = change of the sudut (rad)
  • \sf{\alpha} = angular acceleration (rad/s²)
  • t = interval of the time (s)
  • \sf{\omega_t} = final angular velocity  (rad/s)
  • \sf{\omega_0} =  initial angular velocity (rad/s)

<h2>Problem Solving</h2>

We know that :

  • \sf{\omega_t} = final angular velocity  = 0 rad/s >> see in the sentence "in the process of coming to rest."
  • \sf{\omega_0} =  initial angular velocity = 11 rad/s
  • \sf{\theta} = change of the sudut = 80.0 rad

What was asked :

  • \sf{\alpha} = angular acceleration = ... rad/s²
  • t = interval of the time = ... s

Step by step :

  • \sf{\alpha} = ... rad/s²

\sf{(\omega_t)^2= (\omega_0)^2 + 2 \times \alpha \times \theta}

\sf{0^2= (11)^2 + 2 \times \alpha \times 80}

\sf{0 = 121 + 160 \alpha}

\sf{-160 \alpha = 121}

\sf{\alpha = \frac{121}{-160}}

\sf{\alpha = -0.75625 \: rad/s^2 \approx \boxed{-0.76 \: rad/s^2}}

  • t = ... s

\sf{\alpha = \frac{\omega_0 - \omega_t}{t}}

\sf{-0.76 = \frac{0 - 11}{t}}

\sf{-0.76t = -11}

\sf{t = \frac{- 11}{-0.76}}

\boxed{\sf{t \approx 14.474 \: s}}

<h3>Conclusion</h3>

So :

  • The angular acceleration of the wheel approximately -0.76 rad/s² or proportionally as deceleration approximately 0.76 rad/s.
  • It need approximately 14.474 s to come to rest.
5 0
2 years ago
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