Help understanding Angular V as it applies to Kepler's 2nd law

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The discussion focuses on understanding Kepler's 2nd law as presented in Robert Braeunig's blog on orbital mechanics. A participant struggles with the mathematical description of the area swept by a radius vector during a small time interval, specifically how the height of the triangle relates to angular speed. It is clarified that for small angles, the approximation tan(Δθ) is roughly equal to Δθ, allowing the height to be expressed as rωΔt. The conversation emphasizes that the distance covered along a circular path can be represented as s = rθ, which aids in visualizing the area of the triangle. Overall, the discussion highlights the challenges of grasping these concepts without a calculus background.
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Robert Braeunig has an great blog on rocket science here: http://www.braeunig.us/space/index.htm, and I've been trying to follow the math his piece on Orbital Mechanics.

I'm having trouble in particular following his description on Kepler's 2nd law, here's how he puts it:

fig4-05.gif


Figure 4.5 shows a particle revolving around C along some arbitrary path. The area swept out by the radius vector in a short time interval t is shown shaded. This area, neglecting the small triangular region at the end, is one-half the base times the height or approximately r(rt)/2. This expression becomes more exact as t approaches zero, i.e. the small triangle goes to zero more rapidly than the large one. The rate at which area is being swept out instantaneously is therefore

<br /> \lim_{t\rightarrow 0}{\Big[ \frac{r(rωΔt)}{2} \Big]} = \frac {ωr^2}{2}<br />

I understand the area of the triangle is given by (base x height)/2. I understand r is the triangle base in this case, but how does the opposite side equal rt or rωΔt?

The way I'm reading this is that Angular speed is just change in angle given a change in time ω = Δθ / Δt, so as I understand it, ωΔt just leaves the angle Δθ. So shouldn't the height then be r tan(Δθ)? What am I missing?
 
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I understand the area of the triangle is given by (base x height)/2. I understand r is the triangle base in this case, but how does the opposite side equal rt or rωΔt?

The way I'm reading this is that Angular speed is just change in angle given a change in time ω = Δθ / Δt, so as I understand it, ωΔt just leaves the angle Δθ. So shouldn't the height then be r tan(Δθ)? What am I missing?
For small time periods, ##\tan\Delta\theta \approx \Delta\theta## ... it's an approximation.

The author is giving a description for people who don't have calculus yet.
 
I got hung up by the formula for a triangle in the figure and forgot that the distance covered on a circumference is s = rθ, so it would make sense for it to approximate the height of a very small triangle. Thank you for the reply!
 
Its a common approach - what they really wanted was ##dA=\frac{1}{2}r^2(\theta)d\theta## and you can integrate to get the area swept by motion between two angles.

However, it can take a bit of getting used to.
 
I think it's easist first to watch a short vidio clip I find these videos very relaxing to watch .. I got to thinking is this being done in the most efficient way? The sand has to be suspended in the water to move it to the outlet ... The faster the water , the more turbulance and the sand stays suspended, so it seems to me the rule of thumb is the hose be aimed towards the outlet at all times .. Many times the workers hit the sand directly which will greatly reduce the water...
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