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Firlakuza [10]
3 years ago
7

A body oscillates with simple harmonic motion accordingto the

Physics
1 answer:
gregori [183]3 years ago
8 0

Answer:(a) displacement= 6.0m

(b) velocity = 8.996m/s

(c) acceleration

(d) phase of motion= 2.999

(e) frequency= 1.499hz

(f) period of motion= 0.667sec

Explanation:Given that,

X= (6.0m) cos (3πrad/s)t + π/3rad...(i)

Compare equation (i) to wave equation,

Y= A cos (wt) + kx...(ii)

(a) displacement which is also known as amplitude A. So by comparing equation (i) & (ii), we have A= 6.0m

Therefore,displacement= 6.0m

(b) velocity=B/T (where B= wavelength and T=period)

Wavelength B=2π/k (where k=π/3,comparing the two equations)

Therefore, wavelength B=2π÷π/3=6

Period T= 2π/w (where w=3π,comparing the two equations)

Therefore, period T=2π÷3π=0.667sec

Therefore, Velocity V=B/T=6/0.667=8.996m/s

(d)phase of motion=t/T (where t= elapsed time and T=period)

T=0.667sec ( from (c) solving for velocity)

t=2.0s, as given in the question

Therefore, phase of motion= t/T=2/0.667=2.999

(e) frequency=1/T (where T is the period)

T=0.667secs (recall from (c) while solving for velocity)

Therefore, frequency=1/T=1/0.667=1.499hz

(f) period=1/f (where f= frequency)

Therefore, period=1/f=1/1.499=0.667secs.

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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

              f = 2/2

             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

              R₁ > 0

Cas2 Flat-concave (divergent) lens

             R₂ = infinity

              R₁ <0

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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