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vredina [299]
4 years ago
5

In this diagram of the water cycle, clouds form in the air due to what process? A) run off. B) condensation. C) transpiration. D

) precipitation.
Physics
2 answers:
dezoksy [38]4 years ago
8 0

Answer: Option B, condensation.

Explanation: Clouds are created when vapor of water mixed in the air condensates (because of the lower temperatures and change in pressure) in tiny water drops and ice crystals suspended in the atmosphere, this water drops and ice crystals difract the light of the sun, and this why we see the clouds white. The process in which vapor of water is transformed into liquid water again (or any gas tath transforming into a liquid) is called condensation, so the right answer is B.

Fiesta28 [93]4 years ago
4 0
I can't see the diagram, but it would be condensation. (You can use the process of elimination here as well: precipitation is when rain/snow/sleet/hail falls, run off is.. well, run off, and transpiration is about trees)
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Effciency of a lever is never 100% or more. why?Give reason​
Troyanec [42]

Answer:

Ideally, the work output of a lever should match the work input. However, because of resistance, the output power is nearly always be less than the input power. As a result, the efficiency would go below 100\%.  

Explanation:

In an ideal lever, the size of the input and output are inversely proportional to the distances between these two forces and the fulcrum. Let D_\text{in} and D_\text{out} denote these two distances, and let F_\text{in} and F_\text{out} denote the input and the output forces. If the lever is indeed idea, then:

F_\text{in} \cdot D_\text{in} = F_\text{out} \cdot D_\text{out}.

Rearrange to obtain:

\displaystyle F_\text{in} = F_\text{out} \cdot \frac{D_\text{out}}{D_\text{in}}

Class two levers are levers where the perpendicular distance between the fulcrum and the input is greater than that between the fulcrum and the output. For this ideal lever, that means D_\text{in} > D_\text{out}, such that F_\text{in} < F_\text{out}.

Despite F_\text{in} < F_\text{out}, the amount of work required will stay the same. Let s_\text{out} denote the required linear displacement for the output force. At a distance of D_\text{out} from the fulcrum, the angular displacement of the output force would be \displaystyle \frac{s_\text{out}}{D_\text{out}}. Let s_\text{in} denote the corresponding linear displacement required for the input force. Similarly, the angular displacement of the input force would be \displaystyle \frac{s_\text{in}}{D_\text{in}}. Because both the input and the output are on the same lever, their angular displacement should be the same:

\displaystyle \frac{s_\text{in}}{D_\text{in}} =\frac{s_\text{out}}{D_\text{out}}.

Rearrange to obtain:

\displaystyle s_\text{in}=s_\text{out} \cdot \frac{D_\text{in}}{D_\text{out}}.

While increasing D_\text{in} reduce the size of the input force F_\text{in}, doing so would also increase the linear distance of the input force s_\text{in}. In other words, F_\text{in} will have to move across a longer linear distance in order to move F_\text{out} by the same s_\text{out}.

The amount of work required depends on both the size of the force and the distance traveled. Let W_\text{in} and W_\text{out} denote the input and output work. For this ideal lever:

\begin{aligned}W_\text{in} &= F_\text{in} \cdot s_\text{in} \\ &= \left(F_\text{out} \cdot \frac{D_\text{out}}{D_\text{in}}\right) \cdot \left(s_\text{out} \cdot \frac{D_\text{in}}{D_\text{out}}\right) \\ &= F_\text{out} \cdot s_\text{out} = W_\text{out}\end{aligned}.

In other words, the work input of the ideal lever is equal to the work output.

The efficiency of a machine can be measured as the percentage of work input that is converted to useful output. For this ideal lever, that ratio would be 100\%- not anything higher than that.

On the other hand, non-ideal levers take in more work than they give out. The reason is that because of resistance, F_\text{in} would be larger than ideal:

\displaystyle F_\text{in} = F_\text{out} \cdot \frac{D_\text{out}}{D_\text{in}} + F(\text{resistance}).

As a result, in real (i.e., non-ideal) levers, the work input will exceed the useful work output. The efficiency will go below 100\%,

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3 years ago
The frequency of the musical note F#3 is 1.85x102 hertz. What is its period?
g100num [7]

The period of the musical note is \text { 5. } 4 \times 10^{-3} seconds.

Answer: Option A

<u>Explanation:</u>

The frequency is defined as the number of oscillations or a complete cycle of wave occurred in a given time interval. So the frequency is inversely proportional to the time period. Thus the mathematical representation of frequency with time period is

               \text {Frequency}=\frac{1}{\text {Time period }}

As the frequency is given as 1.85 \times 10^{2} \mathrm{Hz}, the time period can be found as

               \text { Time period }=\frac{1}{\text { Frequency }}

Thus,

               \text { Time period }=\frac{1}{1.85 \times 10^{2}}=5.4 \times 10^{-3} \mathrm{s}

Thus the time period for the frequency of the musical note is \text { 5. } 4 \times 10^{-3} seconds.

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