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/, (r) s + R,fL, 3lfil,fr"## 111#:* gives the transrer function from the input armarure vorrage to the (2nd order system) (1.13) The transfer function from the input armature voltage to the resulting angurar position change is found by multiplying Equation ( I . 13) by ll s .

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  • /, (r)s + R,fL,

    3lfil,fr"## 111#:* gives the transrer function from the input armarure vorrage to the

    (2nd order system) (1.13)

    The transfer function from the input armature voltage to the resulting angurar positionchange is found by multiplying Equation ( I . 13) by ll s .

  • rrG) _

    vf (s)0tL)

    ' +(n,14)

    The transfer function from the inputcombining equations (l .2) and(1.3).

    (1't order system) ( 1.3)

    (1.4)

    voltage to the resulting motor torque is found by

    T*(s) _T*(t) /r(s)

    =Vr(s) t,(s) Vr(s)(x-,lrr)

    s +(n,14) ( 1't order system)

    So, a step input in field voltage results in an exponential rise in the motor torque.

    An equation that describes the rotational motion ofthe inertial load is found by summing moments

    \U - T* - cat * Ja (counterclockwise positive)0r

    Jrh + c0) =T_

    c&=cc9

    Thus, the transfer function from the input motor torqueto rotational speed changes is

    o(s)T^(t) s+(clJ)

    (U J) (1't order system)

    Combining equations (1.4) and (1.5) gives thevoltage to the resulting speed change

    Free Body Diagramof the Inertial Load

    (1.s)

    transfer function from the input field

    Finally, since to -

    d?ldt, the transfer function from input field voltage to the resultingrotational position changb is

    o(s) =

    g(s) T*(t)Vr(s) T^(s) Vr(s)

    (x-r ltrt)

    0(s) 0(s) ar(s)Vr(s) ar(s) I'r(s)

    (x-, ltrt)s(s+clt)(s+RrlLr)

    (2nd order system) (r.6)

    (r.7)

    2

    (3'd order system)

  • Current Controlled:

    In a armature'current controlled motor, the field current7 is held constant, and the armature current is controlledthrough the armature voltage vn. In this case, the motortorque increases linearly with the armature current. wewrite

    T* = K*o io

    The transfer function from the input armature current to theresulting motor torque is

    L"T*el&

    +- V. ---->+

    DC MotorT-(t)ilt) = L*o

    As before, the transfer function from

    a{s) 0tr)4,(s) s +(cl J)

    ( 1.8)

    where [u represents the "back EMF" induced by the rotation of the armature windings in amagnetic field. The back EMF % is proportional to the speed @, i.e. Vub)= qal(s).Taking Laplace transforms of Equation ( I .9) gives

    V,(s) -

    Vub)= (& + z,s)d (s)

    The voltage/current relationship for the armature side of the motor is

    V, =Vo +V, +Vu

    V,(s)- Kua(s) = (& + f,s)f,(s)

    (1.e)

    (1.10)

    (1.12)

    or

    (1.11)

    the input motor torque to rotational speed changes is

    ( I't order system)

    arnr( *uraI*

    Tne,"*,bQ

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