Review Questions and Answers for Chapters 4 and 5 Apes

vii.

(a) 12 m/s 2 12 m/s two .

(b) The dispatch is not one-4th of what information technology was with all rockets burning because the frictional forcefulness is nonetheless every bit large as it was with all rockets called-for.

9.

(a) The system is the child in the wagon plus the wagon.

(b

An object represented as a dot labeled m is shown at the center. One force represented by an arrow labeled as vector F sub 2 acts toward the right. Another force represented by an arrow labeled as vector F sub 1 having a slightly shorter length in comparison with F sub 2 acts on the object pointing left. A friction force represented by an arrow labeled as vector f having a small length acts on the object toward the left. Weight, represented by an arrow labeled as vector W, acts on the object downward, and normal force, represented by an arrow labeled as vector N, acts upward, having the same length as W.

(c) a = 0 . 130 1000/s 2 a = 0 . 130 m/s two size 12{a=0 "." "130"" m/s" rSup { size 8{2} } } {} in the management of the 2d kid's button.

(d) a = 0.00 chiliad/southward 2 a = 0.00 g/s ii size 12{a=0" m/s" rSup { size 8{2} } } {}

11.

(a) 3.68 × ten three Northward three.68 × ten 3 N . This strength is 5.00 times greater than his weight.

(b) 3750 North; xi.3º higher up horizontal 3750 N; 11.3º above horizontal size 12{"3750"" N; xi" "." 3°" above horizontal"} {}

13.

1.5 × ten 3 N , 150 kg , 150 kg one.5 × 10 three N , 150 kg , 150 kg

15.

Strength on shell: 2 . 64 × 10 7 N 2 . 64 × 10 7 N size 12{ii "." "64" times "ten" rSup { size 8{7} } `N} {}

Force exerted on transport = 2 . 64 × 10 7 Northward 2 . 64 × ten 7 N size 12{ - 2 "." "64" times "10" rSup { size viii{seven} } `N} {} , by Newton'south third police force

17.

  1. 0. 11 m/s 2 0. xi chiliad/s ii size 12{0 "." "eleven g/due south" rSup { size 8{2} } } {}
  2. ane . 2 × 10 4 N 1 . ii × ten 4 Northward size 12{i "." 2 times "x" rSup { size 8{4} } " N"} {}

19.

(a) vii . 84 × ten -iv N vii . 84 × x -iv N size 12{seven "." "84" times "10" rSup { size viii{four} } " N"} {}

(b) 1 . 89 × 10 –3 N i . 89 × 10 –iii N size 12{one "." "89" times "10" rSup { size viii{"–3"} } " Due north"} {} . This is 2.41 times the tension in the vertical strand.

21.

Newton's 2nd police force practical in vertical direction gives

F y = F 2 T sin θ = 0 F y = F 2 T sin θ = 0 size 12{F rSub { size 8{y} } =F - 2T" sin "θ=0} {}

F = ii T sin θ F = two T sin θ size 12{F rSub { size eight{ ortho } } =2"T sin "θ} {}

T = F 2 sin θ . T = F 2 sin θ size 12{T= { {F rSub { size 8{ ortho } } } over {"2 sin "θ} } } {} .

23.

An object of mass m is shown. Three forces acting on it are tension T, shown by an arrow acting vertically upward, and friction f and gravity m g, shown by two arrows acting vertically downward.

Using the gratuitous-body diagram:

F net = T f m g = ma F net = T f chiliad g = ma size 12{F rSub { size eight{"net"} } =T - f= ital "ma"} {} ,

so that

a = T f mg 1000 = 1 . 250 × 10 7 Due north 4.50 × ten 6 N ( 5.00 × ten 5 kg ) ( ix. 80 1000/south 2 ) 5.00 × ten 5 kg = half dozen.xx yard/s ii a = T f mg m = ane . 250 × ten vii N four.fifty × 10 6 N ( v.00 × 10 v kg ) ( ix. 80 m/s 2 ) v.00 × ten 5 kg = 6.20 k/s two size 12{a= { {T` - `f` - ` ital "mg"} over {m} } = { {one "." "250" times "10" rSup { size 8{7} } " Northward" - 4 "." "50" times "10" rSup { size 8{"6 "} } Northward - \( 5 "." "00" times "x" rSup { size eight{5} } " kg" \) \( 9 "." "80 k/due south" rSup { size 8{2} } \) } over {five "." "00" times "10" rSup { size 8{5} } " kg"} } ="half dozen" "." 20" chiliad/southward" rSup { size viii{2} } } {} .

25.

  1. Use Newton's laws of movement.
    Two forces are acting on an object of mass m: F, shown by an arrow pointing upward, and its weight w, shown by an arrow pointing downward. Acceleration a is represented by a vector arrow pointing upward. The figure depicts the forces acting on a high jumper.
  2. Given : a = 4.00 g = ( four.00 ) ( ix. 80 yard/south ii ) = 39.2 thousand/s 2 ; a = iv.00 thousand = ( 4.00 ) ( ix. 80 m/s two ) = 39.2 chiliad/s ii ; size 12{a=iv "." "00" chiliad= \( iv "." "00" \) \( 9 "." "80 thou/s" rSup { size 8{2} } \) ="39" "." 2" m/s" rSup { size eight{2} } " ; "} {} one thousand = 70 . 0 kg thousand = lxx . 0 kg size 12{k="70" "." "0 kg"} {} ,

    Notice: F F size 12{F} .

  3. {} {} F =+ F w = ma , F =+ F west = ma , size 12{ Sum {F"=+"F - w= ital "ma"" ,"} } {} and so that F = ma + due west = ma + mg = m ( a + thousand ) F = ma + w = ma + mg = m ( a + g ) size 12{F= ital "ma"+w= ital "ma"+ ital "mg"=m \( a+1000 \) } {} .

    F = ( 70.0 kg ) [ ( 39 . two m/s 2 ) + ( ix . 80 1000/s two ) ] F = ( lxx.0 kg ) [ ( 39 . 2 m/s 2 ) + ( 9 . eighty m/s 2 ) ] size 12{F= \( "70" "." 0" kg" \) \[ \( "39" "." "2 m/s" rSup { size 8{2} } \) + \( 9 "." "80 m/s" rSup { size viii{ii} } \) \] } {} = 3. 43 × 10 3 N = 3. 43 × 10 3 N size 12{ {}= {underline {`3 "." "43" times "ten" rSup { size viii{iii} } " Due north"}} } {} . The force exerted by the high-jumper is really down on the ground, simply F F size 12{F} is up from the basis and makes him jump.

  4. This result is reasonable, since it is quite possible for a person to exert a force of the magnitude of x 3 N 10 3 North size 12{"10" rSup { size 8{3} } " North"} {} .

27.

(a) 4 . 41 × 10 5 Northward 4 . 41 × ten 5 N size 12{4 "." "41" times "10" rSup { size 8{5 } } " Northward"} {}

(b) i . 50 × x five N i . 50 × 10 5 N size 12{1 "." "47" times "10" rSup { size 8{5 } } " N"} {}

29.

(a) 910 N 910 N size 12{"910"N} {}

(b) one . 11 × 10 3 N 1 . 11 × 10 three N size 12{1 "." "xi" times "10" rSup { size 8{three} } " N"} {}

31.

a = 0.139 chiliad/due south a = 0.139 m/due south , θ = 12.4º θ = 12.4º north of eastward

33.

  1. Employ Newton's laws since we are looking for forces.
  2. Depict a forcefulness diagram:
    A horizontal dotted line with two vectors extending downward from the mid-point of the dotted line, both at angles of fifteen degrees. A third vector points straight downward from the intersection of the first two angles, bisecting them; it is perpendicular to the dotted line.
  3. The tension is given every bit T = 25.0 N. T = 25.0 Northward. Find F app . F app . Using Newton's laws gives: Σ F x = 0, Σ F x = 0, so that applied force is due to the y-components of the 2 tensions: F app = two T sin θ = ii ( 25.0 N ) sin ( 15º ) = 12.9 North F app = 2 T sin θ = two ( 25.0 N ) sin ( 15º ) = 12.9 N

    The ten-components of the tension cancel. F 10 = 0 F 10 = 0 .

  4. This seems reasonable, since the applied tensions should be greater than the forcefulness practical to the molar.

40.

10.2 thousand/s 2 , 4.67º from vertical ten.2 m/due south 2 , 4.67º from vertical size 12{"10" "." 2" m/south" rSup { size 8{2} } ", 4" "." "68"°" from vertical"} {}

42.

An object of mass m is shown being pulled by two ropes. Tension T sub two acts toward the right at an angle of ten degrees above the horizontal. Another rope makes an angle fifteen degrees to the left of the vertical direction, and tension in the rope is T sub one, shown by a vector arrow. Weight w is acting vertically downward.

T one = 736 North T 1 = 736 Northward size 12{T rSub { size viii{ane} } ="736"" Due north"} {}

T two = 194 Northward T 2 = 194 N size 12{T rSub { size 8{two} } ="194 Due north"} {}

44.

(a) vii.43 m/southward seven.43 m/s size 12{seven "." "43"" k/south"} {}

(b) 2.97 thousand

46.

(a) iv.xx one thousand/s 4.xx yard/s size 12{4 "." "20"" m/s"} {}

(b) 29.four m/s 2 29.4 m/south 2 size 12{"29" "." 4" chiliad/due south" rSup { size 8{2} } } {}

(c) 4 . 31 × 10 three N 4 . 31 × ten 3 Northward size 12{4 "." "31" times "10" rSup { size eight{3} } " N"} {}

48.

(a) 47.1 k/s

(b) 2 . 47 × 10 3 grand/s 2 ii . 47 × ten three one thousand/s 2 size 12{ii "." "47" times "10" rSup { size viii{3} } " m/south" rSup { size 8{2} } } {}

(c) 6.18 × 10 three North vi.18 × 10 iii N . The average force is 252 times the shell's weight.

52.

(a) 1 × 10 xiii ane × ten 13 size 12{ane times "10" rSup { size viii{ - "13"} } } {}

(b) i × 10 11 ane × x 11 size 12{1 times "ten" rSup { size 8{ - "11"} } } {}

54.

x 2 10 2 size 12{"10" rSup { size 8{two} } } {}

ane.

Motorcar 10 is shown on the left, and Car Y is shown on the right.

i.

Car X takes longer to advance and does not spend whatsoever fourth dimension traveling at summit speed. Motorcar Y accelerates over a shorter time and spends time going at superlative speed. So Car Y must encompass the straightaways in a shorter time. Curves have the same fourth dimension, and so Car Y must overall take a shorter time.

ii.

The just difference in the calculations for the fourth dimension of 1 segment of linear dispatch is the difference in distances. That shows that Car X takes longer to accelerate. The equation d four v c = t c d four v c = t c corresponds to Auto Y traveling for a time at tiptop speed.

Substituting a = v c t 1 a = 5 c t 1 into the displacement equation in part (b) ii gives D = iii ii five c t 1 D = 3 2 5 c t 1 . This shows that a motorcar takes less time to reach its maximum speed when information technology accelerates over a shorter distance. Therefore, Car Y reaches its maximum speed more quickly, and spends more than time at its maximum speed than Car X does, as argued in part (b) i.

iii.

A body cannot exert a force on itself. The militarist may advance as a outcome of several forces. The hawk may accelerate toward Globe as a result of the force due to gravity. The hawk may accelerate every bit a result of the boosted force exerted on it by wind. The hawk may accelerate as a outcome of orienting its body to create less air resistance, thus increasing the internet force forward.

5.

(a) A soccer player, gravity, air, and friction normally exert forces on a soccer ball being kicked.

(b) Gravity and the surrounding h2o commonly exert forces on a dolphin jumping. (The dolphin moves its muscles to exert a force on the water. The water exerts an equal force on the dolphin, resulting in the dolphin's motion.)

(c) Gravity and air exert forces on a parachutist drifting to Globe.

ix.

The diagram consists of a black dot in the centre and two small red arrows pointing up (Fb) and down (Fg) and two long ruby-red arrows pointing correct (Fc = 9.0 N) and left (Fw=13.0 N).

In the diagram, F g represents the force due to gravity on the balloon, and Fb represents the buoyant force. These two forces are equal in magnitude and reverse in management. F c represents the force of the electric current. F w represents the force of the wind. The net force on the balloon volition be F due west F c = iv.0 F w F c = 4.0 N and the balloon will accelerate in the management the wind is blowing.

11.

Since m = F / a one thousand = F / a , the parachutist has a mass of 539 North/9 .viii km/southward ii = 55 kg 539 Due north/9 .8 km/s 2 = 55 kg .

For the commencement ii s, the parachutist accelerates at ix.viii m/s2.

v = a t = 9.8 m s 2 2 s = 19.6 m south five = a t = 9.8 thou due south 2 2 s = 19.vi m s

Her speed after two s is nineteen.half dozen thou/s.

From 2 s to 10 s, the net force on the parachutist is 539 N – 615 Due north, or 76 Northward upward.

a = F m = 76 N 55 kg = 1.iv m s 2 a = F thousand = 76 N 55 kg = 1.4 m southward ii

Since 5 = 5 0 + a t 5 = five 0 + a t , v = nineteen.6 m/s ii + ( 1.four yard/southward 2 ) ( viii s) = 8.4 m/south 2 v = xix.6 yard/due south 2 + ( i.4 one thousand/southward two ) ( 8 s) = 8.4 m/s 2 .

At 10 s, the parachutist is falling to World at 8.four m/s.

thirteen.

The system includes the gardener and the wheelbarrow with its contents. The following forces are important to include: the weight of the wheelbarrow, the weight of the gardener, the normal force for the wheelbarrow and the gardener, the force of the gardener pushing against the ground and the equal forcefulness of the ground pushing dorsum against the gardener, and any friction in the wheelbarrow'southward wheels.

xv.

The system undergoing acceleration is the ii figure skaters together.

Net force = 120 N 5 .0 N = 115 Due north 120 N 5 .0 N = 115 N .

Full mass = xl kg + 50 kg = xc kg 40 kg + 50 kg = 90 kg .

Using Newton's 2nd police force, nosotros have that

a = F m = 115 Northward 90 kg = 1.28 thou s 2 a = F m = 115 Northward 90 kg = 1.28 m s 2

The pair accelerates forward at one.28 m/s2.

17.

The strength of tension must equal the forcefulness of gravity plus the force necessary to accelerate the mass. F = m thousand F = yard g can be used to calculate the first, and F = m a F = m a can be used to summate the second.

For gravity:

F = m g = ( 120.0 kg)(ix .viii m/s ii ) = 1205.iv N F = yard g = ( 120.0 kg)(9 .8 m/southward 2 ) = 1205.4 Due north

For acceleration:

F = thousand a = ( 120.0 kg)(i .iii chiliad/s 2 ) = 159.nine N F = m a = ( 120.0 kg)(i .3 m/s ii ) = 159.ix N

The total forcefulness of tension in the cable is 1176 N + 156 Northward = 1332 Due north.

21.

The diagram has a black dot and three solid red arrows pointing abroad from the dot. Arrow Ft is long and pointing to the left and slightly down. Pointer Fw is also long and is a chip below a diagonal line halfway between pointing up and pointing to the correct. A brusk arrow Fg is pointing downwards.

F g is the force on the kite due to gravity.

F w is the forcefulness exerted on the kite by the wind.

F t is the force of tension in the string belongings the kite. It must remainder the vector sum of the other two forces for the kite to bladder stationary in the air.

27.

A gratuitous-torso diagram would show a northward force of 64 N and a westward strength of 38 N. The net force is equal to the sum of the two applied forces. It can be constitute using the Pythagorean theorem:

F net = F x 2 + F y w = ( 38 N ) ii + ( 64 Northward ) 2 = 74.iv N F cyberspace = F x ii + F y west = ( 38 Northward ) 2 + ( 64 N ) 2 = 74.4 N

Since a = F yard a = F m ,

a = 74.4 N 825 kg = 0.09 m/s two a = 74.iv N 825 kg = 0.09 thou/s ii

The bedrock volition accelerate at 0.09 m/southward2.

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Source: https://openstax.org/books/college-physics-ap-courses/pages/chapter-4

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