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NISA [10]
4 years ago
12

A 24.1 N solid sphere with a radius of 0.151 m is released from rest and rolls, without slipping, 1.7 m down a ramp that is incl

ined at 34o above the horizon. What is the total kinetic energy of the sphere at the bottom of the ramp?What is the angular speed of the sphere at the bottom of the ramp? How many radians did the sphere rotate through as it rolled down the ramp What was the angular acceleration of the sphere as it rolled down the ramp
Physics
1 answer:
damaskus [11]4 years ago
5 0

Answer

given,

weight of solid sphere = 24.1 N

m = 24.1/g  =  24.1/10 = 2.41 Kg

radius = R = 0.151 m

height of the ramp = 1.7 m

angle with horizontal = 34°

acceleration due to gravity = 10 m/s²

using energy conservation

\dfrac{1}{2}I\omega^2 + \dfrac{1}{2}mv^2 = mgh

I for sphere

I = \dfrac{2}{5}mr^2         v = r ω

\dfrac{1}{2}\ \dfrac{2}{5}mr^2\times \dfrac{v^2}{r^2} + \dfrac{1}{2}mv^2 = mgh

\dfrac{7}{10}mv^2 = mgh

h = \dfrac{0.7 v^2}{g}

v = \sqrt{\dfrac{h \times g}{0.7}}

v = \sqrt{\dfrac{1.7 \times 10}{0.7}}

v = 4.93 m/s

b) rotational kinetic energy

KE=\dfrac{1}{2}I\omega^2

KE=\dfrac{1}{2}\ \dfrac{2}{5}mr^2\times \dfrac{v^2}{r^2}

KE=\dfrac{1}{5}mv^2

KE=\dfrac{1}{5}\times 2.41 \times 4.93^2

KE = 11.71 J

c) Translation kinetic energy

KE=\dfrac{1}{2}mv^2

KE=\dfrac{1}{2}\times 2.41 \time 4.93^2

KE=29.28\ J

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1) iii i= 1m, 2)  iii and iv, 3)  i = f₂ (L-f₁) / (L - (f₁ + f₂))

Explanation:

Problem 1

For this problem we use two equations the equations of the focal distance in mirrors

              f = r / 2

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             f = 1 m

The builder's equation

           1 / f = 1 / o + 1 / i

Where f is the focal length, "o and i" are the distance to the object and the image respectively.

For a ray to arrive parallel to the surface it must come from infinity, whereby o = ∞ and 1 / o = 0

              1 / f = 0 + 1 / i

              i = f

              i = 1 m

The image is formed at the focal point

The correct answer is iii

Problem 2

For this problem we have two possibilities the lens is convergent or divergent, in both cases the back face (R₂) must be flat

Case 1 Flat lens - convex (convergent)

              R₂ = infinity

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Cas2 Flat-concave (divergent) lens

             R₂ = infinity

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Why the correct answers are iii and iv

Problem 3

For a thick lens the rays parallel to the first surface fall in their focal length (f₁), this is the exit point for the second surface whereby the distance to the object is o = L –f₁, let's apply the constructor equation to this second surface

          1 / f₂ = 1 / (L-f₁) + 1 / i

          1 / i = 1 / f₂ - 1 / (L-f₁)

           1 / i = (L-f₁-f₂) / f₂ (L-f₁)

           i = f₂ (L-f₁) / (L - (f₁ + f₂))

This is the image of the rays that enter parallel to the first surface

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