1. Velocity at which the packet reaches the ground: 121.2 m/s
The motion of the packet is a uniformly accelerated motion, with constant acceleration
directed downward, initial vertical position
, and initial vertical velocity
. We can use the following SUVAT equation to find the final velocity of the packet after travelling for d=750 m:
![v_f^2 -v_i^2 =2ad](https://tex.z-dn.net/?f=v_f%5E2%20-v_i%5E2%20%3D2ad)
substituting, we find
![v_f^2 = 2ad\\v_f = \sqrt{2ad}=\sqrt{2(9.8 m/s^2)(750 m)}=121.2 m/s](https://tex.z-dn.net/?f=v_f%5E2%20%3D%202ad%5C%5Cv_f%20%3D%20%5Csqrt%7B2ad%7D%3D%5Csqrt%7B2%289.8%20m%2Fs%5E2%29%28750%20m%29%7D%3D121.2%20m%2Fs)
2. height at which the packet has half this velocity: 562.6 m
We need to find the heigth at which the packet has a velocity of
![v_f=\frac{121.2 m/s}{2}=60.6 m/s](https://tex.z-dn.net/?f=v_f%3D%5Cfrac%7B121.2%20m%2Fs%7D%7B2%7D%3D60.6%20m%2Fs)
In order to do that, we use again the same SUVAT equation substituting
with this value, so that we find the new distance d that the packet travelled from the helicopter to reach this velocity:
![v_f^2-v_i^2=2ad\\d=\frac{v_f^2}{2a}=\frac{(60.6 m/s)^2}{2(9.8 m/s^2)}=187.4 m](https://tex.z-dn.net/?f=v_f%5E2-v_i%5E2%3D2ad%5C%5Cd%3D%5Cfrac%7Bv_f%5E2%7D%7B2a%7D%3D%5Cfrac%7B%2860.6%20m%2Fs%29%5E2%7D%7B2%289.8%20m%2Fs%5E2%29%7D%3D187.4%20m)
Which means that the heigth of the packet was
![h=750 m-187.4 m=562.6 m](https://tex.z-dn.net/?f=h%3D750%20m-187.4%20m%3D562.6%20m)
The change in distance is 30 because if you subtract both number you'll get 30
The Asthenosphere is where the convection currents in the Earth occor
Answer:
I think its (A)The specific heat of an object explains how easily it changes temperatures.
Explanation:
Answer:
Yes
Explanation:
There are two types of interference possible when two waves meet at the same point:
- Constructive interference: this occurs when the two waves meet in phase, i.e. the crest (or the compression, in case of a longitudinale wave) meets with the crest (compression) of the other wave. In such a case, the amplitude of the resultant wave is twice that of the original wave.
- Destructive interferece: this occurs when the two waves meet in anti-phase, i.e. the crest (or the compression, in case of a longitudinal wave) meets with the trough (rarefaction) of the other wave. In this case, the amplitude of the resultant wave is zero, since the amplitudes of the two waves cancel out.
In this problem, we have a situation where the compression of one wave meets with the compression of the second wave, so we have constructive interference.