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Georgia [21]
3 years ago
7

Anyone can help?? I need this done before 9am please!!

Physics
1 answer:
pav-90 [236]3 years ago
8 0

Answer:

The slopes for each of the four line segments are a_{A} = 6\,\frac{m}{min^{2}}, a_{B} = 0\,\frac{m}{min^{2}}, a_{C} = -4\,\frac{m}{min^{2}} and a_{D} = 2.667\,\frac{m}{min^{2}}, respectively.

Explanation:

There are four line segments:

(i) Line A: v(0\,min) = 0\,\frac{m}{min}, v(10\,min) = 60\,\frac{m}{min}

(ii) Line B: v(10\,min) = 60\,\frac{m}{min}, v(15\,min) = 60\,\frac{m}{min}

(iii) Line C: v(15\,min) = 60\,\frac{m}{min}, v(40\,min) = -40\,\frac{m}{min}

(iv) Line D: v(40\,min) = -40\,\frac{m}{min}, v(55\,min) = 0\,\frac{m}{min}

The slope of each line segment represents the acceleration of the particle, which can calculated by the geometrical concept of secant line. Hence, we proceed to determine the acceleration associated with each line segment:

Line A

a_{A} = \frac{v(10\,min)-v(0\,min)}{10\,min-0\,min}

a_{A} = \frac{60\,\frac{m}{min}-0\,\frac{m}{min}}{10\,min-0\,min}

a_{A} = 6\,\frac{m}{min^{2}}

Line B

a_{B} = \frac{v(15\,min)-v(10\,min)}{15\,min-10\,min}

a_{B} = \frac{60\,\frac{m}{min}-60\,\frac{m}{min}  }{15\,min-10\,min}

a_{B} = 0\,\frac{m}{min^{2}}

Line C

a_{C} = \frac{v(40\,min)-v(15\,min)}{40\,min-15\,min}

a_{C} = \frac{-40\,\frac{m}{min}-60\,\frac{m}{min}  }{40\min-15\,min}

a_{C} = -4\,\frac{m}{min^{2}}

Line D

a_{D} = \frac{v(55\,min)-v(40\,min)}{55\,min-40\,min}

a_{D} = \frac{0\,\frac{m}{min}-\left(-40\,\frac{m}{min} \right) }{55\,min-40\,min}

a_{D} = 2.667\,\frac{m}{min^{2}}

The slopes for each of the four line segments are a_{A} = 6\,\frac{m}{min^{2}}, a_{B} = 0\,\frac{m}{min^{2}}, a_{C} = -4\,\frac{m}{min^{2}} and a_{D} = 2.667\,\frac{m}{min^{2}}, respectively.

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f'=(\frac{v+v_r}{v+v_s})f

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f is the apparent frequency

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v_s is the velocity of the source (positive if the source is moving away from the receiver, negative otherwise)

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f = 1110 Hz

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In the reflector frame (= on surface B), we have also

v_s = v_A = -28.7 m/s (surface A is the source, which is moving towards the receiver)

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So, the frequency observed in the reflector frame is

f'=(\frac{334 m/s+62.2 m/s}{334 m/s-28.7 m/s})1110 Hz=1440.5 Hz

(b) 0.232 m

The wavelength of a wave is given by

\lambda=\frac{v}{f}

where

v is the speed of the wave

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In the reflector frame,

f = 1440.5 Hz

So the wavelength is

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(c) 1481.2 Hz

Again, we can use the same formula

f'=(\frac{v+v_r}{v+v_s})f

In the source frame (= on surface A), we have

v_s = v_B = -62.2 m/s (surface B is now the source, since it reflects the wave, and it is moving towards the receiver)

v_r = +28.7 m/s (surface A is now the receiver, which is moving towards the source)

So, the frequency observed in the source frame is

f'=(\frac{334 m/s+28.7 m/s}{334 m/s-62.2 m/s})1110 Hz=1481.2 Hz

(d) 0.225 m

The wavelength of the wave is given by

\lambda=\frac{v}{f}

where in this case we have

v = 334 m/s

f = 1481.2 Hz is the apparent in the source frame

So the wavelength is

\lambda=\frac{334 m/s}{1481.2 Hz}=0.225 m

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