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Drag Force Calculations

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Road Cycling
Published
18 October 2005
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18 October 2005
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Paul Hobson
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  1. In going over some old hydraulics notes for a current class, I stumbled
    across a problem I worked calculating the drag force and power output
    required for a cyclist at various headwinds. I threw it all into
    MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul
    --
    Paul M. Hobson
    Georgia Institute of Technology
    ..:change the words to numbers
    if you want to reply to me:.

  2. Paul Hobson <[email hidden]> wrote in news:dj1hnf$75p$1@news-
    int.gatech.edu:

    Quoted message said:

    In going over some old hydraulics notes for a current class, I stumbled
    across a problem I worked calculating the drag force and power output
    required for a cyclist at various headwinds. I threw it all into
    MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul

    I'm not going to question your math, but the power values look awfully high
    to me. I frequently ride at 20 mph into a 10 mph wind, and my CD is way
    higher than racing cyclist. And that's not counting the "inefficiency" of
    the bike, like getting the wheels to centripitally accelerate. In other
    words, I really don't think I'm putting out 450 - 500 watts in a real
    situation. If I am, find me a trireme, I'd love to go on a nice cruise 😉

    --ag

  3. Andy Gee said:

    Paul Hobson <[email hidden]> wrote in news:dj1hnf$75p$1@news-
    int.gatech.edu:

    Quoted message said:

    In going over some old hydraulics notes for a current class, I stumbled
    across a problem I worked calculating the drag force and power output
    required for a cyclist at various headwinds. I threw it all into
    MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul

    I'm not going to question your math, but the power values look awfully high
    to me. I frequently ride at 20 mph into a 10 mph wind, and my CD is way
    higher than racing cyclist. And that's not counting the "inefficiency" of
    the bike, like getting the wheels to centripitally accelerate. In other
    words, I really don't think I'm putting out 450 - 500 watts in a real
    situation. If I am, find me a trireme, I'd love to go on a nice cruise 😉

    --ag

    Hmm...it was an example problem worked in class -- originally in US
    units. In that MathCad worksheet, I got the same answer as the
    professor, which was 0.047 hp for the tail wind and 0.422 hp for the
    head wind, respectively. According to both MathCad, my HP-48G+
    calculator <heart>, and myself with conversion factors, those figures
    roughly translate to 35.1 W and 315.5 W (I rounded the velocities to
    nice even numbers so the two versions don't exactly translate).

    The situation at you mention -- going at 20 mph with a 10 mph headwind
    -- would correspond to an output of 315.5 W, which is somewhat lower
    than the 450 W to 500 W range that you mention. Yes, it does seem high.
    But 20 mph with a 10 mph headwind is not an easy situation. Quite
    impressive, really. Lastly, keep in mind that the SI chart's x-axis is
    in kph (kilometers per hour).

    ....

    Any better?
    --
    Paul M. Hobson
    Georgia Institute of Technology
    ..:change the words to numbers
    if you want to reply to me:.

  4. Paul Hobson said:

    Any thoughts? Gross errors?

    How come it requires .2 hp to go zero MPH? Shouldn't it require 0 HP?

  5. Rich said:
    Paul Hobson said:

    Any thoughts? Gross errors?

    How come it requires .2 hp to go zero MPH? Shouldn't it require 0 HP?

    In the second graph (right?), 0 mph is the velocity of the *air*
    relative to the *ground*. Thus, the air would be moving at 20 mph
    relative to the cyclist.

    --
    Paul M. Hobson
    Georgia Institute of Technology
    ..:change the words to numbers
    if you want to reply to me:.

  6. Paul Hobson said:

    In going over some old hydraulics notes for a current class, I stumbled
    across a problem I worked calculating the drag force and power output
    required for a cyclist at various headwinds. I threw it all into
    MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul

    These calculators are all over the net, why not cross check against them?

  7. Peter Cole said:
    Paul Hobson said:

    In going over some old hydraulics notes for a current class, I
    stumbled across a problem I worked calculating the drag force and
    power output required for a cyclist at various headwinds. I threw it
    all into MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul

    These calculators are all over the net, why not cross check against them?

    Oh, I had no idea. [googles]

    --
    Paul M. Hobson
    Georgia Institute of Technology
    ..:change the words to numbers
    if you want to reply to me:.

  8. Paul Hobson said:

    In going over some old hydraulics notes for a current class, I stumbled
    across a problem I worked calculating the drag force and power output
    required for a cyclist at various headwinds. I threw it all into
    MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul

    What are the same values for temperatures other than ~60 F? I bike
    at temperatures from -15 to 90. Drag force is really much more
    noticeable at higher density -- although maybe it's because I
    present a larger cross-section to the wind.

    Scott

  9. Scott said:
    Paul Hobson said:

    In going over some old hydraulics notes for a current class, I
    stumbled across a problem I worked calculating the drag force and
    power output required for a cyclist at various headwinds. I threw it
    all into MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul

    What are the same values for temperatures other than ~60 F? I bike
    at temperatures from -15 to 90. Drag force is really much more
    noticeable at higher density -- although maybe it's because I
    present a larger cross-section to the wind.

    Drag coefficients are independent of the fluid in which bodies are
    submerged. To account for different temperatures, the density simply
    needs to be changed using the Ideal Gas Law:

    density = (P*M)/(R*T)
    with
    P = pressure (kPa or lbf/ft^2)
    M = molecular weight of air = 28.97 kg/kmol = lbm/lbmol
    R = 8.314 kJ/kmol*K = 1545 lbf/lbmol * degrees Rankine
    T = temperature in Kelvins or degrees Rankine as appropriate

    Since the power output is directly proportional to the density, simply
    multiply the final answers on my sheet by the ratio of your calculated
    density over the one I used.

    I also found this:

    Area (ft^2) C_D
    upright commuter 5.5 1.1
    racing 3.9 0.88
    drafting 3.9 0.50
    streamlined* 5.0 0.12

    * the illustration for this is a very simple silhouette of a recumbent
    with what I guess us some sort of cage that they use in those
    human-powered speed competitions. it doesn't really explain the
    values at all.
    --
    Paul M. Hobson
    Georgia Institute of Technology
    ..:change the words to numbers
    if you want to reply to me:.

  10. Paul Hobson said:
    Scott said:
    Paul Hobson said:

    In going over some old hydraulics notes for a current class, I
    stumbled across a problem I worked calculating the drag force and
    power output required for a cyclist at various headwinds. I threw it
    all into MathCad really fast so I could share. I added some graphs too.

    If you're awesome and use the metric system:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm

    If you prefer US units:
    http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm

    Any thoughts? Gross errors?

    \\paul

    What are the same values for temperatures other than ~60 F? I bike
    at temperatures from -15 to 90. Drag force is really much more
    noticeable at higher density -- although maybe it's because I
    present a larger cross-section to the wind.

    Drag coefficients are independent of the fluid in which bodies are
    submerged. To account for different temperatures, the density simply
    needs to be changed using the Ideal Gas Law:

    density = (P*M)/(R*T)
    with
    P = pressure (kPa or lbf/ft^2)
    M = molecular weight of air = 28.97 kg/kmol = lbm/lbmol
    R = 8.314 kJ/kmol*K = 1545 lbf/lbmol * degrees Rankine
    T = temperature in Kelvins or degrees Rankine as appropriate

    Since the power output is directly proportional to the density, simply
    multiply the final answers on my sheet by the ratio of your calculated
    density over the one I used.

    I also found this:

    Area (ft^2) C_D
    upright commuter 5.5 1.1
    racing 3.9 0.88
    drafting 3.9 0.50
    streamlined* 5.0 0.12

    * the illustration for this is a very simple silhouette of a recumbent
    with what I guess us some sort of cage that they use in those
    human-powered speed competitions. it doesn't really explain the values
    at all.

    Very interesting. I really do find it much more difficult
    to bike in the ~10% denser air of winter than summer and
    have always assumed it's because of greater drag in the
    denser air, rather than the effect of density on the power
    ouput. Incidentally, I guess I'm the upright commuter --
    and in winter with bulky clothes, the cross-section is a
    lot higher. So it's a combination of the two.

    Scott

  11. Scott said:
    Paul Hobson said:
    Scott said:

    Paul Hobson wrote:

    > In going over some old hydraulics notes for a current class, I
    > stumbled across a problem I worked calculating the drag force and
    > power output required for a cyclist at various headwinds. I threw
    > it all into MathCad really fast so I could share. I added some
    > graphs too.
    >
    > If you're awesome and use the metric system:
    > http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm
    >
    > If you prefer US units:
    > http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm
    >
    > Any thoughts? Gross errors?
    >
    > \\paul

    What are the same values for temperatures other than ~60 F? I bike
    at temperatures from -15 to 90. Drag force is really much more
    noticeable at higher density -- although maybe it's because I
    present a larger cross-section to the wind.

    Drag coefficients are independent of the fluid in which bodies are
    submerged. To account for different temperatures, the density simply
    needs to be changed using the Ideal Gas Law:

    density = (P*M)/(R*T)
    with
    P = pressure (kPa or lbf/ft^2)
    M = molecular weight of air = 28.97 kg/kmol = lbm/lbmol
    R = 8.314 kJ/kmol*K = 1545 lbf/lbmol * degrees Rankine
    T = temperature in Kelvins or degrees Rankine as appropriate

    Since the power output is directly proportional to the density, simply
    multiply the final answers on my sheet by the ratio of your calculated
    density over the one I used.

    I also found this:

    Area (ft^2) C_D
    upright commuter 5.5 1.1 racing 3.9 0.88
    drafting 3.9 0.50
    streamlined* 5.0 0.12

    sorry about the crappy formatting -- it looked better when I typed it up.

    Quoted message said:
    Quoted message said:

    * the illustration for this is a very simple silhouette of a recumbent
    with what I guess us some sort of cage that they use in those
    human-powered speed competitions. it doesn't really explain the
    values at all.

    Very interesting. I really do find it much more difficult
    to bike in the ~10% denser air of winter than summer and
    have always assumed it's because of greater drag in the
    denser air

    you're right, it is.

    Quoted message said:

    rather than the effect of density on the power
    ouput.

    and you are right there too!

    Quoted message said:

    Incidentally, I guess I'm the upright commuter --
    and in winter with bulky clothes, the cross-section is a
    lot higher. So it's a combination of the two.

    The denser air increases the drag force, which /then/ increases the
    required power output. So, AFAIK, you were correct in your initial
    assessment.

    Drag Force is proportional to air density.
    Power output is proportional to drag force, therefore
    Power output is proportional to air density. make sense?

    --
    Paul M. Hobson
    Georgia Institute of Technology
    ..:change the words to numbers
    if you want to reply to me:.

  12. Paul Hobson said:
    Scott said:
    Paul Hobson said:

    Scott wrote:

    > Paul Hobson wrote:
    >
    >> In going over some old hydraulics notes for a current class, I
    >> stumbled across a problem I worked calculating the drag force and
    >> power output required for a cyclist at various headwinds. I threw
    >> it all into MathCad really fast so I could share. I added some
    >> graphs too.
    >>
    >> If you're awesome and use the metric system:
    >> http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_SI.htm
    >>
    >> If you prefer US units:
    >> http://www.prism.gatech.edu/~gtg611a/bike_calcs/drag_net_us.htm
    >>
    >> Any thoughts? Gross errors?
    >>
    >> \\paul
    >
    >
    >
    >
    >
    > What are the same values for temperatures other than ~60 F? I bike
    > at temperatures from -15 to 90. Drag force is really much more
    > noticeable at higher density -- although maybe it's because I
    > present a larger cross-section to the wind.

    Drag coefficients are independent of the fluid in which bodies are
    submerged. To account for different temperatures, the density simply
    needs to be changed using the Ideal Gas Law:

    density = (P*M)/(R*T)
    with
    P = pressure (kPa or lbf/ft^2)
    M = molecular weight of air = 28.97 kg/kmol = lbm/lbmol
    R = 8.314 kJ/kmol*K = 1545 lbf/lbmol * degrees Rankine
    T = temperature in Kelvins or degrees Rankine as appropriate

    Since the power output is directly proportional to the density,
    simply multiply the final answers on my sheet by the ratio of your
    calculated density over the one I used.

    I also found this:

    Area (ft^2) C_D
    upright commuter 5.5 1.1 racing 3.9 0.88
    drafting 3.9 0.50
    streamlined* 5.0 0.12

    sorry about the crappy formatting -- it looked better when I typed it up.

    Quoted message said:
    Quoted message said:

    * the illustration for this is a very simple silhouette of a
    recumbent with what I guess us some sort of cage that they use in
    those human-powered speed competitions. it doesn't really explain
    the values at all.

    Very interesting. I really do find it much more difficult
    to bike in the ~10% denser air of winter than summer and
    have always assumed it's because of greater drag in the
    denser air

    you're right, it is.

    Quoted message said:

    rather than the effect of density on the power
    ouput.

    and you are right there too!

    Oops -- I read 'drag coefficients are independent of fluid'
    as 'drag is independent of fluid' -- which didn't make sense.

    Never mind!!!

    scott

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