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Science Forum Forum Index » Physics » misUnderstand Gragh of ball moving with resistence of the ai

  
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ArezList
Posted: Wed Jul 09, 2008 8:31 pm    Post subject: misUnderstand Gragh of ball moving with resistence of the ai Reply with quote

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Hi all

Here is a question:

a ball with the mass M is thrown with the angle of Δ,and a the initial vleocity of V, the air resistenec is propositonal with V(2){V square}, namely: Resistence= kV(2), K is a constant. The acceleration of gravitivity is g (m/s2)

Question: what is the Velocity and displacement chart , compare to the graph without air resistence?


Undersatnd the question ? sorry for my english.... By the way can someone analyse it with equations shown, thank you very much!
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Harold14370
Posted: Thu Jul 10, 2008 2:01 am    Post subject: Reply with quote

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Try this article.

http://en.wikipedia.org/wiki/Trajectory_of_a_projectile
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Cold Fusion
Posted: Thu Jul 10, 2008 2:41 am    Post subject: Reply with quote

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While the ball would fall a little faster (depending on various factors in an atmosphere....whether it is dimpled, its weight, shape) in a vacuum, it would also have less resistance to travel in the horizontal direction. So, it could potentially land in a very similar spot to the one in an atmosphere.

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Undersatnd the question ? sorry for my english....


And yet you still give him a wikipedia article? Surprised
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Last edited by Cold Fusion on Thu Jul 10, 2008 4:15 pm; edited 1 time in total
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ArezList
Posted: Thu Jul 10, 2008 4:29 am    Post subject: Reply with quote

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ok that's fine but

which will take longer time rising(T1) or falling(T2),

then if we define that without air resistence the time of ball rising is T,
what's the relations between T1 and T, and also T2 and T?

By the way does my english too poor, or already poor enough?
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Harold14370
Posted: Thu Jul 10, 2008 5:21 am    Post subject: Reply with quote

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ArezList wrote:
ok that's fine but

which will take longer time rising(T1) or falling(T2),

then if we define that without air resistence the time of ball rising is T,
what's the relations between T1 and T, and also T2 and T?

By the way does my english too poor, or already poor enough?


Did you look at the chart in the wikipedia article? It has the answer to your question.
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JaneBennet
Posted: Thu Jul 10, 2008 8:30 pm    Post subject: Reply with quote

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Harold, the Wikipedia article is assuming that air resistance is proportional to the velocity; this problem in this thread is assuming is assuming it’s proportional to the square of the velocity. The two problems are different.
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Last edited by JaneBennet on Fri Jul 11, 2008 5:47 am; edited 2 times in total
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JaneBennet
Posted: Thu Jul 10, 2008 10:05 pm    Post subject: Re: misUnderstand Gragh of ball moving with resistence of th Reply with quote

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ArezList wrote:
a ball with the mass M is thrown with the angle of Δ,and a the initial vleocity of V, the air resistenec is propositonal with V(2){V square}, namely: Resistence= kV(2), K is a constant. The acceleration of gravitivity is g (m/s2)

Question: what is the Velocity and displacement chart , compare to the graph without air resistence!

From what I’ve worked through of the question so far, it looks like the answers are not going to be pretty-looking … Shocked

You have v^2=v_x^2+v_y^2, where v_x and v_y are respectively the horizontal and vertical components of the velocity.

Then \dfrac{dv_x}{dt} and \dfrac{dv_y}{dt} are respectively the horizontal and vertical components of the acceleration. The forceNow consider the horizontal and vertical forces on the ball:

Horizontally: M\dfrac{dv_x}{dt}=-kv_x^2

Vertically: M\dfrac{dv_y}{dt}=\left\{\begin{array}{ll}-Mg-kv_y^2 & \mbox{going up}\\\\-Mg+kv_y^2 & \mbox{coming down}\end{array}

Each of the differential equations to be solved is of the variables-separable kind.

For the horizontal case, the solution is v_x=\dfrac{M}{C_x+kt}, where C_x is a constant. At time t=0, v_x=V_0\cos{\Delta} (assuming the angle is with respect to the horizontal); therefore C_x=\dfrac{M}{V_0\cos{\Delta}}. Hence v_x=\dfrac{MV_0\cos{\Delta}}{M+(kV_0\cos{\Delta})t}.

Similarly, solve the differential equations for v_y, then substitute v_x and v_y into v=\pm\sqrt{v_x^2+v_y^2} to get your velocity–time relations.

For the displacement–time relations, use v=\dfrac{ds}{dt}.
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