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beks73 [17]
4 years ago
14

If there is an attractive force between all objects, why do we not feel ourselves gravitating toward massive buildings in our vi

cinity?
Physics
2 answers:
mars1129 [50]4 years ago
8 0
The mass of an object affects how powerful the attractive force is. To feel the pull / gravitation the mass of the object would have to be huge, bigger than that of massive buildings
HACTEHA [7]4 years ago
4 0
Because there is a far more massive nearby object that's attracting you to it. That object is the planet you're standing on. Compared to its mass, that massive building could just as well be a speck of dust or a clump of lint. The gravitational attraction toward Earth completely swamps out the attraction toward anything else.
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Read 2 more answers
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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