The magnet incessant wheel

نوشته شده در موضوع تولید انرژی رایگان در 27 نوامبر 2017
  • Creation date: 11th of August. 2012

    The incessant circle driven by a permanent magnet

    The inventor

    The judgment of this incessant circle has been law in 1823.

    That invention is entirely described in book “Mechanical Appliances and Novelties of Construction” published in 1927 by Gardner D. Hiscox, Mechanical Engineer, and Norman W. Henley.

    The engine described in a video herebelow is of a comparatively elementary design.

    Description of a invention concept

    A clever magnet set in a open container between sides of a circle attracts an iron ball.

    The magnet is ostensible to pull a round to one side of a core to make a circle henceforth unbalanced.

    It is critical to note that a immobile intensity appetite of a captivating force is converted into pristine kinetic energy.


    Theoretical investigate of a incessant wheel

    We assume that a round rolls and slips on a middle lane of
    the wheel.

    The several inventoried waste of this engine are :

    • Rolling attrition waste ( Rrf ) of a round on a middle lane of a circle and ensuing from internal deformation of a raceway underneath a weight of a ball,
    • Power waste due to shifting of a hit surfaces of a round and raceway (ω’ is larger than ω),
    • Loss of dual round orientation commissioned on a pivot of a wheel.


    Balance of forces

    Balance of army along y1 pivot :

    Balance of army along x1 pivot :

    We have a following attribute between Rrf and R :

    Then, it comes:

    Expressing a following equalities :

    It comes afterwards :

    In this formula, a following terms are known: F magnet, m, g, α and θ. α is a angle of a rolling friction.

    The combined
    gravity and captivating army means an craze of a rolling round which
    is not compensated by an equal and conflicting greeting force. The round is
    forced to stagger and this revolution drives a categorical circle by means of
    rolling attrition force.

    Due to defilement of Newton’s third law, there is origination of additional certain appetite from intensity appetite granted by immobile captivating and gravitic

    Static intensity appetite is so converted into kinetic appetite by that incessant wheel.


    Calculation of expostulate torque

    The expostulate torque is equal to Tdrive = Fresulting x r , soit:


    Calculation of estuary power

    Excepting parasitic movements related to immediate instabilities of operation and holding a arrogance of a consistent angle theta, one can determine that a captivating and sobriety army yield no appetite to mechanism. These dual army are concerned usually in progressing an inconstant state. Then:


    Calculation of expostulate power

    The shifting fellow rslip of a round on a middle competition of a circle is voiced by a following formula:

    , afterwards :

    Let’s calculate a expostulate appetite : Pdrive = Tdrive . ω’


    Let’s calculate a opening appetite : Poutlet = Fresulting . R . ω

    It has to be remarkable that:

    and :


    Calculation of COP (coefficient of performance)

    Pnet outlet = Poutlet– Pwheel attrition losses

    Pwheel attrition losses = 1% Poutlet and

    Pnet outlet = 0,99 Poutlet



    Calculation of COE (coefficient of energy)


    Numerical application

    r = 0,015 m – R = 0,15 m – g = 9,81 m/s² – θ = 30° – tan α = 0,001 – r slip = 10% – ω = 60 rpm = 6,2832 rd/s – B = 0,4 T – μ0 = 4 π 10-7 – μr = 1,0000004 – S = 0,01 x 0,01 = 10-4

    Fmagnet = 6,366 N

    m = 0,014 kg

    Fresulting = 5,442 N

    Tdrive = 0,041 mN

    Pdrive = 5,700 W

    Poutlet = 5,130 W

    P rolling losses = 0,570 W

    P net outlet = 5,078 W

    P circle attrition losses = 0,052 W

    COP = ∞

    COE = ∞


    Improved mechanism

    An softened pattern of a resource would include to appurtenance teethed surfaces on a middle lane of a circle and a outdoor aspect of a executive partial of a cylinder (ball transposed by a cylinder). Each finish of a cylinder has a rolling cylindrical aspect of same hole as a rigging representation hole on executive part.

    Thus, a shifting of a dual hit surfaces is cancelled and a operation of a circle is some-more stable.

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