Ball rolls down ramp, ball is released from spring, ball drops down chute.
To solve this problem we will apply the relation of Ohm's law, at the same time we will use the concept of resistance in a cable, resistivity and potential difference.
According to Ohm's law we have to
![V= IR](https://tex.z-dn.net/?f=V%3D%20IR)
Here,
V = Voltage
I = Current
R = Resistance
At the same time resistance can be described as
![R = \frac{\rho l}{A}](https://tex.z-dn.net/?f=R%20%3D%20%5Cfrac%7B%5Crho%20l%7D%7BA%7D)
Here,
= Resistivity of the material
l = Length of the specimen
A = Cross-sectional area
From the above expression we can write the current as,
![I = \frac{V}{R}](https://tex.z-dn.net/?f=I%20%3D%20%5Cfrac%7BV%7D%7BR%7D)
![I = \frac{V}{\frac{\rho l}{A}}](https://tex.z-dn.net/?f=I%20%3D%20%5Cfrac%7BV%7D%7B%5Cfrac%7B%5Crho%20l%7D%7BA%7D%7D)
![I =\frac{VA}{\rho l}](https://tex.z-dn.net/?f=I%20%3D%5Cfrac%7BVA%7D%7B%5Crho%20l%7D)
Replacing we have that,
![I = \frac{(0.8V)(0.4*10^{-6}m^2)}{(5.6*10^{-8}\Omega \cdot m)(1.5m)}](https://tex.z-dn.net/?f=I%20%3D%20%5Cfrac%7B%280.8V%29%280.4%2A10%5E%7B-6%7Dm%5E2%29%7D%7B%285.6%2A10%5E%7B-8%7D%5COmega%20%5Ccdot%20m%29%281.5m%29%7D)
![I = 3.809A](https://tex.z-dn.net/?f=I%20%3D%203.809A)
Therefore the current in the wire is 3.809A
<em>Note: The value obtained for the resistivity of Tungsten was theoretically obtained and can be consulted online.</em>
Answer:
A
Explanation:
Snell's law states:
n₁ sin θ₁ = n₂ sin θ₂
where n is the index of refraction and θ is the angle of incidence (relative to the normal).
The index of refraction of air is approximately 1. So:
1 sin 30° = 1.52 sin θ
θ ≈ 19°
Answer:
bounced back at oncoming waves
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If the incoming wave strikes a barrier at a 90 degree angle, the wave energy is, in fact bouncing back at oncoming waves.
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Hope this helps!