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082-Engineering-Mathematics-Anthony-Croft-Robert-Davison-Martin-Hargreaves-James-Flint-Edisi-5-2017

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72 Chapter 2 Engineering functions

Note that the voltage is a linear polynomial function with I as the independent

variable.

This equation is only valid for a finite range of currents. If too much voltage is

appliedtotheresistor,thenthecurrentflowingthroughtheresistorbecomessufficient

forthe resistortooverheat and breakdown.

Engineeringapplication2.5

Anon-idealvoltagesource

An ideal voltage source has zero internal resistance and its output voltage,V, is independent

of the load applied to it; that is,V remains constant, independent of the

current it supplies. It is called an ideal voltage source because it is difficult to create

such a source in practice; it is in effect an abstraction that is useful when developing

engineering models of real electronic systems. A non-ideal voltage source has

aninternal resistance. Due tothis internal resistance, the output voltage from such a

source is reduced when current is drawn from the source. The voltage reduction increasesasmorecurrentisdrawn.Figure2.18showsanon-idealvoltagesource.Itis

modelledasanidealvoltagesourceinserieswithaninternalresistorwithresistance

R s

. The output voltage of the non-ideal voltage source is v o

while v R

is the voltage

drop across the internal resistor andiis the load current. Using Kirchhoff’s voltage

law,

V=v R

+v o

and hence by Ohm’s law,

V =iR s

+v o

v o

=V−iR s

Note thatV and R s

are constants and so the output voltage is a linear polynomial

function with independent variable i. The equation gives the output voltage across

theloadasafunctionofthecurrentthroughtheload.Theoutputcharacteristicforthe

non-idealvoltagesourceisobtainedbyvaryingtheloadresistorR L

andisplottedin

Figure2.19.Noticethattheoutputvoltageofthenon-idealvoltagesourcedecreases

as the load current increases and is equal in value to the ideal voltage source only

when there isno load current.

V

+

R s

v R

v o

i

R L

v o

V

gradient = –R s

i

non-ideal voltage source

Figure2.18

Anon-ideal voltage sourceconnected to aload

resistor,R L .

Figure2.19

Output characteristic ofanon-ideal

voltage source.

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