Fundamentals of Electric Circuits
Fundamentals of Electric Circuits
6th Edition
ISBN: 9780078028229
Author: Charles K Alexander, Matthew Sadiku
Publisher: McGraw-Hill Education
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Chapter 6, Problem 85CP

A square-wave generator produces the voltage waveform shown in Fig. 6.94(a). What kind of a circuit component is needed to convert the voltage waveform to the triangular current waveform shown in Fig. 6.94(b)? Calculate the value of the component, assuming that it is initially uncharged.

Figure 6.94

For Prob. 6.85.

Chapter 6, Problem 85CP, A square-wave generator produces the voltage waveform shown in Fig. 6.94(a). What kind of a circuit , example  1

Chapter 6, Problem 85CP, A square-wave generator produces the voltage waveform shown in Fig. 6.94(a). What kind of a circuit , example  2

Expert Solution & Answer
Check Mark
To determine

Find the circuit component that is needed to convert the voltage waveform into the triangular current waveform and to calculate the value of the circuit component.

Answer to Problem 85CP

The circuit component inductor is needed to convert the given voltage waveform into the triangular current waveform and the value for the inductor (L) is 1.25mH.

Explanation of Solution

Given data:

Refer to Figure 6.94 in the textbook.

Formula used:

Write the expression to calculate the straight line equation for two points (x1,y1) and (x2,y2).

(yy1)=y2y1x2x1(xx1) (1)

Refer to Figure 6.94(b) in the textbook.

From the given graph, substitute t for x and i for y in equation (1).

(iy1)=y2y1x2x1(tx1) (2)

Calculation:

The given voltage waveform is redrawn as Figure 1.

Fundamentals of Electric Circuits, Chapter 6, Problem 85CP , additional homework tip  1

The given triangular current waveform is redrawn as Figure 2.

Fundamentals of Electric Circuits, Chapter 6, Problem 85CP , additional homework tip  2

Refer to Figure 1 and Figure 2. Generally, integration of the square waveform gives the triangular waveform. That is, the integration of the voltage waveform gives the current waveform. Such relation can be obtained in following relation.

i=1Lvdt (3)

Here,

i is the current through the inductor,

L is the value of the inductor, and

v is the voltage across the inductor.

Refer to equation (3), the circuit component inductor is needed to convert the square voltage waveform to the triangular current waveform.

Differentiate the equation (3) with respect to t to find didt.

didt=ddt(1Lvdt)=1L(ddtvdt)=vL

Rearrange the above equation to find v.

v=Ldidt (4)

Refer to Figure 1. The voltage function is expressed as,

v={5V, 0ms<t<1ms5V, 1ms<t<2ms5V, 2ms<t<3ms5V, 3ms<t<4ms (5)

Refer to Figure 2, split up the time period as four divisions 0ms<t<1ms, 1ms<t<2ms, 2ms<t<3ms and 3ms<t<4ms to find the respective current value.

Case (i): 0ms<t<1ms

The two points (x1,y1) and (x2,y2) are (0ms,0A) and (1ms,4A).

Substitute 0ms for x1, 0A for y1, 1ms for x2 and 4A for y2 in equation (2).

(i0A)=4A0A1ms0ms(t0ms)=4A1mst=4A1×103t {1m=103}=4000tA

Simplify the equation to find i.

i=4000tA+0A=4000tA

Case (ii): 1ms<t<2ms

The two points (x1,y1) and (x2,y2) are (1ms,4A) and (2ms,0A).

Substitute 1ms for x1, 4A for y1, 2ms for x2 and 0A for y2 in equation (2).

(i4A)=0A4A2ms1ms(t1ms)=4A1ms(t1ms)=4A1×103(t(1×103)) {1m=103}=4000(t0.001)A

Simplify the equation to find i.

i=4000tA+4A+4A=4000tA+8A=(84000t)A

Case (iii): 2ms<t<3ms

The two points (x1,y1) and (x2,y2) are (2ms,0A) and (3ms,4A).

Substitute 2ms for x1, 0A for y1, 3ms for x2 and 4A for y2 in equation (2).

(i0A)=4A0A3ms2ms(t2ms)=4A1ms(t2ms)=4A1×103(t(2×103)) {1m=103}=4000(t0.002)A

Simplify the equation to find i.

i=4000tA8A+0A=4000tA8A=(4000t8)A

Case (iv): 3ms<t<4ms

The two points (x1,y1) and (x2,y2) are (3ms,4A) and (4ms,0A).

Substitute 3ms for x1, 4A for y1, 4ms for x2 and 0A for y2 in equation (2).

(i4A)=0A4A4ms3ms(t3ms)=4A1ms(t3ms)=4A1×103(t(3×103)) {1m=103}=4000(t0.003)A

Simplify the equation to find i.

i=4000tA+12A+4A=4000tA+16A=(164000t)A

Therefore, the current function of the signal in Figure 2 is,

i={4000tA, 0ms<t<1ms(84000t)A, 1ms<t<2ms(4000t8)A, 2ms<t<3ms(164000t)A, 3ms<t<4ms

For 0ms<t<1ms:

Substitute 4000tA for i in equation (4) to find v.

v=Ld(4000tA)dt=L(4000)ddt(t)A=4000L(1)As=4000LAs

For 1ms<t<2ms:

Substitute (84000t)A for i in equation (4) to find v.

v=Ld((84000t)A)dt=Lddt(84000t)A=L(04000(1))As=4000LAs

For 2ms<t<3ms:

Substitute (4000t8)A for i in equation (4) to find v.

v=Ld((4000t8)A)dt=Lddt(4000t8)A=L(4000(1)0)As=4000LAs

For 3ms<t<4ms:

Substitute (164000t)A for i in equation (4) to find v.

v=Ld((164000t)A)dt=Lddt(164000t)A=L(04000(1))As=4000LAs

Therefore, the voltage function of the Figure 2 is expressed as,

v={4000LAs, 0ms<t<1ms4000LAs, 1ms<t<2ms4000LAs, 2ms<t<3ms4000LAs, 3ms<t<4ms (6)

The voltage function of the signal in Figure 1 is equal to the voltage function that is obtained in equation (6).

Compare the equations (5) and (6) for any of the time limits. Assume the comparison is made for 0ms<t<1ms.

4000LAs=5V

Rearrange the above equation to find L.

L=(54000)VsA=0.00125H {1H=1V1s1A}=0.00125×103×103H=1.25mH {1m=103}

Therefore, the circuit component inductor is needed to convert the given voltage waveform into the triangular current waveform and the value for the inductor (L) is 1.25mH.

Conclusion:

Thus, the circuit component inductor is needed to convert the given voltage waveform into the triangular current waveform and the value for the inductor (L) is 1.25mH.

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