HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions.pdf · 2013-03-03 · HW #...

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HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions 1.20 Find complex numbers t = z 1 + z 2 and s = z 1 – z 2 , both in polar form, for each of the following pairs: a) z 1 = 2 + j3 and z 2 = 1 – j2 b) z 1 = 3 and z 2 = -j3 c) z 1 = 430° and z 2 = 3-30° d) z 1 = 330° and z 2 = 3-150° a) z 1 + z 2 = 2 + j3 + 1 – j2 = 3 + j = ( ) = 18.43° z 1 – z 2 = 2 + j3 – 1 + j2 = 1 + j5 = ( )= 78.7° b) z 1 + z 2 = 3 – j3 = ( ) = 4.24-45° z 1 - z 2 = 3 + j3 = ( ) = 4.2445° c) z 1 + z 2 = 330° + 3-30° = () () ( )=5.190 z 1 - z 2 = 330° - 3-30°= () () ( )=390 d) z 1 + z 2 =330° + 3-150°= () () =0 z 1 - z 2 =330° - 3-150°= () () ( )=630

Transcript of HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions.pdf · 2013-03-03 · HW #...

Page 1: HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions.pdf · 2013-03-03 · HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions 1.20 Find complex

HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011

Solutions

1.20 Find complex numbers t = z1 + z2 and s = z1 – z2, both in polar form, for each of the following

pairs:

a) z1 = 2 + j3 and z2 = 1 – j2

b) z1 = 3 and z2 = -j3

c) z1 = 430° and z2 = 3-30°

d) z1 = 330° and z2 = 3-150°

a) z1 + z2 = 2 + j3 + 1 – j2 = 3 + j = √ ( ) = √ 18.43°

z1 – z2 = 2 + j3 – 1 + j2 = 1 + j5 = √ ( )= √ 78.7°

b) z1 + z2 = 3 – j3 = √ ( ) = 4.24-45°

z1 - z2 = 3 + j3 = √ ( ) = 4.2445°

c) z1 + z2 = 330° + 3-30° = ( ) ( )

√ (

)=5.190

z1 - z2 = 330° - 3-30°= ( ) ( )

√ ( )=390

d) z1 + z2 =330° + 3-150°= ( ) ( )

=0

z1 - z2 =330° - 3-150°= ( ) ( )

√ (

)=630

Page 2: HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions.pdf · 2013-03-03 · HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions 1.20 Find complex

1.25 A voltage source is given by ( ) ( ) is connected to a series RC

load as shown is Fig. 1-20. If R = 1 MΩ and C = 200pF, obtain an expression for ( ), the voltage

across the capacitor.

Essentially, this is a voltage divider, for which

, where Rpartial is the amount

of resistance taking place after the point of the Vout measurement. However, since this uses a

capacitor, one must use complex resistance values (also known as impedance), which will be

noted here with a Z.

From Table 1-5,

√( ) (

)

√( )

( )

√( ) (

( ))|

( ) ( )

3.2 Given vectors , show that C is

perpendicular to both A and B.

Two vectors are perpendicular if their dot product is 0.

Page 3: HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions.pdf · 2013-03-03 · HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions 1.20 Find complex

3.9 Find an expression for the unit vector directed toward the origin from an arbitrary point on the

line described by x = 1 and z = -3.

The unit vector to be found is depicted, in red, by this figure:

At any point along this line, a vector pointing away from the origin is given by the coordinates of

the point:

.

To reverse the direction, and thus point towards the origin, one needs only to take the negative of

each vector component:

To make this a unit vector, divide by the magnitude:

√ ( )

√ ( )

Page 4: HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions.pdf · 2013-03-03 · HW # 1: 1.20, 1.25, 3.2, 3.9, 3.26, 3.33 - Due Sept. 9, 2011 Solutions 1.20 Find complex

3.26 Find the volumes described by

a) ⁄

b) ⁄

a) This can be solved by algebra. One need only to take the volume of a cylinder of radius 5

and height 2 and subtract from it the volume of a cylinder of radius 2 and height 2, which

gives ( ) . Additionally, a radial variance from ⁄

corresponds to only one quadrant, which means only one fourth of this volume should be

counted. ⁄ ⁄

b) With density assumed to be 1, the integral in spherical coordinates takes the form:

∫ ∫ ∫

∫ ∫

|

∫ ∫

∫ |

|

3.33 Transform the vector into cylindrical coordinates

and then evaluate it at ( ⁄ ⁄ ).

From table 3-2: and

√ ( ⁄ ) .

So, ( ) ( )

( ) ( )

( ( ( ⁄ )) ( ( ⁄ )))

( ( ( ⁄ )) ( ( ⁄ ))

( ( ⁄ )))

Since ⁄ and ⁄ , all terms cancel out except the