Answer:
21 m/s.
Explanation:
The computation of the wind velocity is shown below:
But before that, we need to find out the angles between the vectors
53° - 35° = 18°
Now we have to sqaure it i.e given below
v^2 = 55^2 + 40^2 - 2 · 55 · 40 · cos 18°
v^2 = 3025 + 1600 - 2 · 55 · 40 · 0.951
v^2 = 440.6
v = √440.6
v = 20.99
≈ 21 m/s
Hence, The wind velocity is 21 m/s.
I am pretty sure that <span>the following whihc cannot be determined by looking at the phase diagram is definitely </span>D. system pressure. I consider this one to be correct because only this point is not included into<span> phase diagram and can't be determined itself. Hope it will help! Regards!</span>
When an object absorbs an amount of energy equal to Q, its temperature raises by
![\Delta T](https://tex.z-dn.net/?f=%5CDelta%20T)
following the formula
![Q=m C_s \Delta T](https://tex.z-dn.net/?f=Q%3Dm%20C_s%20%5CDelta%20T)
where m is the mass of the object and
![C_s](https://tex.z-dn.net/?f=C_s%20)
is the specific heat capacity of the material.
In our problem, we have
![Q=2.44 \cdot 10^3 J](https://tex.z-dn.net/?f=Q%3D2.44%20%5Ccdot%2010%5E3%20J)
,
![m=235.0 g](https://tex.z-dn.net/?f=m%3D235.0%20g)
and
![\Delta T=35 K](https://tex.z-dn.net/?f=%5CDelta%20T%3D35%20K)
, so we can re-arrange the formula and substitute the numbers to find the specific heat capacity of the metal:
Answer:
a) f ’’ = f₀
, b) Δf = 2 f₀ ![\frac{v}{c}](https://tex.z-dn.net/?f=%5Cfrac%7Bv%7D%7Bc%7D)
Explanation:
a) This is a Doppler effect exercise, which we must solve in two parts in the first the emitter is fixed and in the second when the sound is reflected the emitter is mobile.
Let's look for the frequency (f ’) that the mobile aorta receives, the blood is leaving the aorta or is moving towards the source
f ’= fo
This sound wave is reflected by the blood that becomes the emitter, mobile and the receiver is fixed.
f ’’ = f’
where c represents the sound velocity in stationary blood
therefore the received frequency is
f ’’ = f₀
let's simplify the expression
f ’’ = f₀ \frac{c+v}{c-v}
f ’’ = f₀
b) At the low speed limit v <c, we can expand the quantity
(1 -x)ⁿ = 1 - x + n (n-1) x² + ...
f ’’ = fo
f ’’ = fo ![( 1 + 2 \frac{v}{c} + \frac{v^2}{ c^2} )](https://tex.z-dn.net/?f=%28%201%20%2B%202%20%5Cfrac%7Bv%7D%7Bc%7D%20%2B%20%5Cfrac%7Bv%5E2%7D%7B%20c%5E2%7D%20%29)
leave the linear term
f ’’ = f₀ + f₀ 2
the sound difference
f ’’ -f₀ = 2f₀ v/c
Δf = 2 f₀ ![\frac{v}{c}](https://tex.z-dn.net/?f=%5Cfrac%7Bv%7D%7Bc%7D)
Answer:
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Explanation: