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Anon25 [30]
3 years ago
12

A narrow beam of light containing red (660 nm) and blue (470 nm) wavelengths travels from air through a 1.00-cm-thick flat piece

of crown glass and back to air again. The beam strikes at a 30.0° incident angle.
(a) At what angles do the two colors emerge?
(b) By what distance are the red and blue separated when they emerge?
Physics
1 answer:
nlexa [21]3 years ago
5 0

Answer

given,

wavelength of red light = 660 nm

wavelength of blue light = 470 nm

thickness = 1 cm = 0.01 m

angle of incident = 30°

using Snell's law

n₁ sin θ₁ = n₂ sin θ₂

refractive index for red and blue color for crown glass

n_r = 1.512     n_b = 1.524

now,

incident ray is red

sin (\theta_{ir})=\dfrac{1\times sin(30^0)}{1.512}

when incident ray is blue

sin (\theta_{ib})=\dfrac{1\times sin(30^0)}{1.524}

so,

(\theta_e)_r=sin^{-1}(\dfrac{1.512 sin (\theta_{ir})}{1})

(\theta_e)_r=sin^{-1}(\dfrac{1.512\times \dfrac{1\times sin(30^0)}{1.512}}{1})

on solving

(\theta_e)_r = 30^0

similarly for blue ray the angle of emerge is 30°

b)

now, refracting angle of blue and red ray

sin (\theta_{ir})=\dfrac{1\times sin(30^0)}{1.512}

\theta_{ir}=19.316^0

for blue ray

sin (\theta_{ib})=\dfrac{1\times sin(30^0)}{1.524}

\theta_{ib}=19.158^0

now,

 d₁ = 1 x tan(19.316°) = 0.3505 m

 d₂ = 1 x tan (19.158°) = 0.3474 m

now, the distance is separated by

  Δ d = d₁ - d₂

  Δ d = 0.3505 - 0.3474

 Δ d =0.0031 cm

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Flow rate of air is given as 83.33 cubic feet per minute

Explanation:

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How does electrical conduction compare between metals, nonmetals, and metalloids
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Answer:

metal> metalloids >nonmetals    (Electrical conductivity)

Explanation:

Electrical conductivity of objects can be compared by the bonding energy of electrons in them.

Metals have less bonding energy of electrons, so even at room temperature their are significant number of free electrons to carry electrical current.

Nonmetals have a very high bonding energy of electrons, so  at room temperature negligible number of free electrons are present so electrical conductivity is very low.

Metalloids have both metallic and non metallic features. The electron bonding energy falls in between that of metals and nonmetals. So electrical conductivity also lies in between metals and nonmetals.

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A baseball pitcher throws a ball at 97.0 mi/h in the horizontal direction. How far does the ball fall vertically by the time it
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Answer:

Explanation:

1 mile=5280 ft

1 hour=3600 seconds

Changing speed from mi/h to ft/s

97 mi/h \times \frac {5280}{3600}=142.2666667 ft/s\approx 142.27 ft/s

Time of flight, t=\frac {distance}{speed}=\frac {60.5}{142.27}=0.425257732 s\approx 0.425 s

From fundamental kinematics equations

h=0.5gt^{2} where g is acceleration due to gravity whose value is taken as 32.2 ft/s2 and h is the distance

By substitution

h=0.5\times 32.2\times 0.425^{2}=2.9080625 m\approx 2.91 m

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3 years ago
In an engine, a piston oscillates with simple harmonic motion so that its position varies according to the following expression,
eduard

(a) 4.06 cm

In a simple harmonic motion, the displacement is written as

x(t) = A cos (\omega t + \phi) (1)

where

A is the amplitude

\omega is the angular frequency

\phi is the phase

t is the time

The displacement of the piston in the problem is given by

x(t) = (5.00 cm) cos (5t+\frac{\pi}{5}) (2)

By putting t=0 in the formula, we find the position of the piston at t=0:

x(0) = (5.00 cm) cos (0+\frac{\pi}{5})=4.06 cm

(b) -14.69 cm/s

In a simple harmonic motion, the velocity is equal to the derivative of the displacement. Therefore:

v(t) = x'(t) = -\omega A sin (\omega t + \phi) (3)

Differentiating eq.(2), we find

v(t) = x'(t) = -(5 rad/s)(5.00 cm) sin (5t+\frac{\pi}{5})=-(25.0 cm/s) sin (5t+\frac{\pi}{5})

And substituting t=0, we find the velocity at time t=0:

v(0)=-(25.00 cm/s) sin (0+\frac{\pi}{5})=-14.69 cm/s

(c) -101.13 cm/s^2

In a simple harmonic motion, the acceleration is equal to the derivative of the velocity. Therefore:

a(t) = v'(t) = -\omega^2 A cos (\omega t + \phi)

Differentiating eq.(3), we find

a(t) = v'(t) = -(5 rad/s)(25.00 cm/s) cos (5t+\frac{\pi}{5})=-(125.0 cm/s^2) cos (5t+\frac{\pi}{5})

And substituting t=0, we find the acceleration at time t=0:

a(0)=-(125.00 cm/s) cos (0+\frac{\pi}{5})=-101.13 cm/s^2

(d) 5.00 cm, 1.26 s

By comparing eq.(1) and (2), we notice immediately that the amplitude is

A = 5.00 cm

For the period, we have to start from the relationship between angular frequency and period T:

\omega=\frac{2\pi}{T}

Using \omega = 5.0 rad/s and solving for T, we find

T=\frac{2\pi}{5 rad/s}=1.26 s

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3 years ago
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