Momentum and electricity problems and solutions
POWER IN ELECTRIC CIRCUITS 
푃 = 퐼푉 푃 훼 퐼, 푉 푐표푛푠푡푎푛푡, 푒푠푝푒푐푖푎푙푙푦 푖푛 푝푎푟푎푙푙푒푙 푐푖푟푐푢푖푡푠 
ℎ푒푛푐푒: 푡ℎ푒 푙표푤푒푟 푟푒푠푖푠푡표푟 풃풖풓풏풔 풃풓풊품풉풕풆풓 
P = 퐼2푅 푃 훼 푅, 퐼 푐표푛푠푡푎푛푡 푖푛 푠푒푟푖푒푠 푐푖푟푐푢푖푡 , 
HENCE, LOWER RESISTOR BURNS DIM 
푃 = 
푉2 
푅 
(푃 훼 푉2), 푅 푐표푛푠푡푎푛푡
PROBLEM 65 CHAPTER 20 
Information to use 
• When two or more resistors are in series, the equivalent resistance is given by 
Rs  R1  R2  R3  . . . 
• When resistors are in parallel, the expression to be solved to find the equivalent resistance is given by 
1 
Rp 
 
1 
R1 
 
1 
R2 
 
1 
R3 
 ... 
. 
We will successively apply these to the individual resistors in the figure in the text 
beginning with the resistors on the right side of the figure. 
• Since the 4.0- and the 6.0- resistors are in series, the equivalent resistance of the combination of those two resistors is 10.0 . 
• The 9.0- and 8.0- resistors are in parallel; their equivalent resistance is 4.24 . 
• The equivalent resistances of the parallel combination (9.0  and 8.0 ) and the series combination (4.0  and the 6.0 ) are in parallel; equivalent resistance is 2.98 . 
. 
• The 2.98- combination is in series with the 3.0- resistor, so that equivalent resistance is 5.98 . 
• Finally, the 5.98- combination and the 20.0- resistor are in parallel, so the equivalent resistance between the points A and B is 4.6  
Related problem no 64 page 632
PROBLEM 85 CHAPTER 20 
STEP 1: CHOOSE A JUNCTION AND DIRECTIONS OF CURRENTS AND ALLOCATE SIGNS ON RESISTORS 
STEP 2: APPLY THE JUNCTION RULE : 
푰ퟏ + 푰ퟑ = 푰ퟐ … … … … … … (ퟏ) 
STEP 3: APPLYING THE LOOP RULE 
LOOP ABCD CLOCKWISE: 
−ퟐ 푰ퟏ + ퟔ푽 + ퟒ 푰ퟑ + ퟑ푽 = ퟎ … … … … … ퟐ 
LOOP BEFC CLOCKWISE: 
−ퟖ 푰ퟐ − ퟗ 푽 − ퟒ 푰ퟑ − ퟔ푽 = ퟎ … … … … … ퟑ 
SOLVING SIMULTANEOUS EQUATIONS WE GET 
푰ퟑ = −ퟏ. ퟖퟐ 푨 
SIGNIFICANCE OF MINUS SIGN: 
+ B 
+ 
+ + + 
3.00 V 9.00 V 
C 
6.00 V 
A 
D 
E 
F 
2.00 Ω 
8.00 Ω 
I1 I2 
I3 4.00 Ω 
+ 
The minus sign indicates that the current in the 4.00- resistor is directed downward , rather 
than upward as selected arbitrarily in the drawing.
CHAPTER 7: PROBLEM 25
REASONING 
• No net external force acts on the plate parallel to the floor; therefore, the 
component of the momentum of the plate that is parallel to the floor is 
conserved as the plate breaks and flies apart. 
• Initially, the total momentum parallel to the floor is zero. After the collision 
with the floor, the component of the total momentum parallel to the floor 
must remain zero. 
• The drawing in the text shows the pieces in the plane parallel to the floor just 
after the collision. 
• Clearly, the linear momentum in the plane parallel to the floor has two 
components; therefore the linear momentum of the plate must be conserved 
in each of these two mutually perpendicular directions. 
• Using the drawing in the text, with the positive directions taken to be up and 
to the right, we have 
m v  m v  1 1 2 2 (sin 25.0 ) + (cos 45.0 ) = 0 
(1) 
y direction m v m v m v 1 1 2 2 3 3 (cos 25.0) + (sin 45.0) – = 0 
(2) 
Substituting known values and solving equations simultaneously we get 
m1  1.00 kg 
m2  1.00 kg 
. 
Related example 9 section 7.4 in your prescribed book: Cutnell and Johnsons 9th Edition

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Momentum and electricity problems and solutions

  • 2. POWER IN ELECTRIC CIRCUITS 푃 = 퐼푉 푃 훼 퐼, 푉 푐표푛푠푡푎푛푡, 푒푠푝푒푐푖푎푙푙푦 푖푛 푝푎푟푎푙푙푒푙 푐푖푟푐푢푖푡푠 ℎ푒푛푐푒: 푡ℎ푒 푙표푤푒푟 푟푒푠푖푠푡표푟 풃풖풓풏풔 풃풓풊품풉풕풆풓 P = 퐼2푅 푃 훼 푅, 퐼 푐표푛푠푡푎푛푡 푖푛 푠푒푟푖푒푠 푐푖푟푐푢푖푡 , HENCE, LOWER RESISTOR BURNS DIM 푃 = 푉2 푅 (푃 훼 푉2), 푅 푐표푛푠푡푎푛푡
  • 3. PROBLEM 65 CHAPTER 20 Information to use • When two or more resistors are in series, the equivalent resistance is given by Rs  R1  R2  R3  . . . • When resistors are in parallel, the expression to be solved to find the equivalent resistance is given by 1 Rp  1 R1  1 R2  1 R3  ... . We will successively apply these to the individual resistors in the figure in the text beginning with the resistors on the right side of the figure. • Since the 4.0- and the 6.0- resistors are in series, the equivalent resistance of the combination of those two resistors is 10.0 . • The 9.0- and 8.0- resistors are in parallel; their equivalent resistance is 4.24 . • The equivalent resistances of the parallel combination (9.0  and 8.0 ) and the series combination (4.0  and the 6.0 ) are in parallel; equivalent resistance is 2.98 . . • The 2.98- combination is in series with the 3.0- resistor, so that equivalent resistance is 5.98 . • Finally, the 5.98- combination and the 20.0- resistor are in parallel, so the equivalent resistance between the points A and B is 4.6  Related problem no 64 page 632
  • 4. PROBLEM 85 CHAPTER 20 STEP 1: CHOOSE A JUNCTION AND DIRECTIONS OF CURRENTS AND ALLOCATE SIGNS ON RESISTORS STEP 2: APPLY THE JUNCTION RULE : 푰ퟏ + 푰ퟑ = 푰ퟐ … … … … … … (ퟏ) STEP 3: APPLYING THE LOOP RULE LOOP ABCD CLOCKWISE: −ퟐ 푰ퟏ + ퟔ푽 + ퟒ 푰ퟑ + ퟑ푽 = ퟎ … … … … … ퟐ LOOP BEFC CLOCKWISE: −ퟖ 푰ퟐ − ퟗ 푽 − ퟒ 푰ퟑ − ퟔ푽 = ퟎ … … … … … ퟑ SOLVING SIMULTANEOUS EQUATIONS WE GET 푰ퟑ = −ퟏ. ퟖퟐ 푨 SIGNIFICANCE OF MINUS SIGN: + B + + + + 3.00 V 9.00 V C 6.00 V A D E F 2.00 Ω 8.00 Ω I1 I2 I3 4.00 Ω + The minus sign indicates that the current in the 4.00- resistor is directed downward , rather than upward as selected arbitrarily in the drawing.
  • 6. REASONING • No net external force acts on the plate parallel to the floor; therefore, the component of the momentum of the plate that is parallel to the floor is conserved as the plate breaks and flies apart. • Initially, the total momentum parallel to the floor is zero. After the collision with the floor, the component of the total momentum parallel to the floor must remain zero. • The drawing in the text shows the pieces in the plane parallel to the floor just after the collision. • Clearly, the linear momentum in the plane parallel to the floor has two components; therefore the linear momentum of the plate must be conserved in each of these two mutually perpendicular directions. • Using the drawing in the text, with the positive directions taken to be up and to the right, we have m v  m v  1 1 2 2 (sin 25.0 ) + (cos 45.0 ) = 0 (1) y direction m v m v m v 1 1 2 2 3 3 (cos 25.0) + (sin 45.0) – = 0 (2) Substituting known values and solving equations simultaneously we get m1  1.00 kg m2  1.00 kg . Related example 9 section 7.4 in your prescribed book: Cutnell and Johnsons 9th Edition