mcastillo356
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- Homework Statement
- The frequency of a car horn is ##400\,\text{Hz}##. If the horn is honked as the car moves with speed ##u_s=34\,\text{m/s}## through still air toward a stationary receiver, find ##(a)## the wavelenth of the sound passing the receiver, and ##(b)## the frequency recieved. Take the speed of sound in air as ##343\,\text{m/s}##. ##(c)##Find the wavelength of the sound passing the receiver and find the frequency received if the car is stationary as the horn is honked and a receiver moves with a speed ##u_r=34\,\text{m/s}## toward the car.
- Relevant Equations
- ##\lambda=\cfrac{v-u_s}{f_s}##
##f_r=\cfrac{v\pm{u_r}}{v\pm{u_s}}\,f_s##
##\lambda=\cfrac{v\pm{u_s}}{f_s}##
PICTURE ##(a)## The waves in front of the source are compressed, so we use the minus sign in ##\lambda=(v\pm{u_s})/f_s##. ##(b)## We calculate the received frequency using ##f_r=[(v\pm{u_r})/(v\pm{u_s})]f_s##. ##(c)## For a moving receiver, we use the same equations as in Parts ##(a)## and ##(b)##.
SOLVE
Calculate the wavelength in front of the car. In front of the source the wavelength is shorter, so choose the sign accordingly:
$$\lambda=\cfrac{v-u_s}{f_s}=\cfrac{343\,\text{m/s}-34\,\text{m/s}}{400\,\text{Hz}}=0.758\,\text{m}=\boxed{0.76\,\text{m}}$$
Solve for the received frequency with ##u_r=0##
$$f_r=\cfrac{v\pm{u_r}}{v\pm{u_s}}\,f_s=\cfrac{v}{v-u_s}\,f_s=\Bigg (\cfrac{343}{343-34}\Bigg )(400\,\text{Hz})=453\,\text{Hz}=450\,\text{Hz}$$
Why the sign minus in the second equation?
##(c)## 1. Calculate the wavelength in front of the source with ##u_s=0##
$$\lambda=\cfrac{v\pm{u_s}}{f_s}=\cfrac{343\,\text{m/s}}{400\,\text{Hz}}=0858\,\text{m}=\boxed{0.86\,\text{m}}$$
2. The received frequency is given with ##u_s##. The source is approaching the receiver, so the frequency is shifted upward. Choose the sign accordingly:
$$f_r=\cfrac{v\pm{u_r}}{v\pm{u_s}}\,f_s=\cfrac{v+u_r}{v}\,f_s=\Bigg (1+\cfrac{u_r}{v}\Bigg )\,f_s=\Bigg (1+\cfrac{34}{343}\Bigg )(400\,\text{Hz})=\boxed{440\,\text{Hz}}$$
In front of the source the wavelength is shorter. Why then is bigger than the wavelength in front of the car?
SOLVE
Calculate the wavelength in front of the car. In front of the source the wavelength is shorter, so choose the sign accordingly:
$$\lambda=\cfrac{v-u_s}{f_s}=\cfrac{343\,\text{m/s}-34\,\text{m/s}}{400\,\text{Hz}}=0.758\,\text{m}=\boxed{0.76\,\text{m}}$$
Solve for the received frequency with ##u_r=0##
$$f_r=\cfrac{v\pm{u_r}}{v\pm{u_s}}\,f_s=\cfrac{v}{v-u_s}\,f_s=\Bigg (\cfrac{343}{343-34}\Bigg )(400\,\text{Hz})=453\,\text{Hz}=450\,\text{Hz}$$
Why the sign minus in the second equation?
##(c)## 1. Calculate the wavelength in front of the source with ##u_s=0##
$$\lambda=\cfrac{v\pm{u_s}}{f_s}=\cfrac{343\,\text{m/s}}{400\,\text{Hz}}=0858\,\text{m}=\boxed{0.86\,\text{m}}$$
2. The received frequency is given with ##u_s##. The source is approaching the receiver, so the frequency is shifted upward. Choose the sign accordingly:
$$f_r=\cfrac{v\pm{u_r}}{v\pm{u_s}}\,f_s=\cfrac{v+u_r}{v}\,f_s=\Bigg (1+\cfrac{u_r}{v}\Bigg )\,f_s=\Bigg (1+\cfrac{34}{343}\Bigg )(400\,\text{Hz})=\boxed{440\,\text{Hz}}$$
In front of the source the wavelength is shorter. Why then is bigger than the wavelength in front of the car?