GRADE 10 PRACTICE
Physics Problems: Dynamics, Grade 10
Newton's laws and fundamental forces.
Here the conditions and analysis of the solution can be read without an account. In the simulator, you need to collect the same analyzes yourself: “Given,” formulas, order of steps and answer.
Problem statements
The answer options are there to check against, and the walkthrough opens under each problem.
Problem #35
Dynamics: Newton's lawsWhat force must be applied to a lead block of volume 40\,\text{см}^{3}so that it moves with acceleration 5\,\text{м/с}^{2}? How much will a dynamometer spring stretch? 120\,\text{Н/м}, if you hang this block from it? Lead density 11300 kg/m³; in the first experiment the applied force is the resultant one.
Show the walkthroughHide the walkthrough
- V
- 40\,\text{см}^{3}=40\cdot 10^{-6}\,\text{м}^{3}
- \rho
- 11{,}3\,\tfrac{\text{г}}{\text{см}^{3}}=11\,300\,\tfrac{\text{кг}}{\text{м}^{3}}
- a
- 5\,\tfrac{\text{м}}{\text{с}^{2}}
- k
- 120\,\tfrac{\text{Н}}{\text{м}}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
F - ?\Delta \ell - ?
- m = \rho Vm = 11{,}3\,\tfrac{\text{г}}{\text{см}^{3}}\cdot 40\,\text{см}^{3}452\,\text{г} = 0{,}452\,\text{кг}
- F = maF = 0{,}452\,\text{кг}\cdot 5\,\tfrac{\text{м}}{\text{с}^{2}}F = 2{,}26\,\text{Н}
- F_{\text{т}} = mgF_{\text{т}} = 0{,}452\cdot 10F_{\text{т}} = 4{,}52\,\text{Н}
The same block hangs on the spring, so it is stretched by gravity.
- F_{\text{у}} = k\Delta\ell\ \Rightarrow\ \Delta\ell = \dfrac{F_{\text{т}}}{k}\Delta\ell = \dfrac{4{,}52\,\text{Н}}{120\,\tfrac{\text{Н}}{\text{м}}}0{,}0377\,\text{м} \approx 3{,}8\,\text{см}
AnswerF = 2{,}26\,\text{Н}\Delta\ell = 0{,}0377\,\text{м}
Problem #36
Dynamics: Newton's lawsForce imparts mass to a body m_1 acceleration a_1, and a body of mass m_2 - acceleration a_2. What acceleration will this force impart to a body of mass m_1+m_2?
Show the walkthroughHide the walkthrough
- m_1
- m_1,\ a_1
- m_2
- m_2,\ a_2
a - ?
- m_1 = \dfrac{F}{a_1},\quad m_2 = \dfrac{F}{a_2}
The force is the same, so we express the masses through it.
- m = m_1 + m_2 = \dfrac{F}{a_1} + \dfrac{F}{a_2} = \dfrac{F\left(a_1 + a_2\right)}{a_1 a_2}
- a = \dfrac{F}{m} = \dfrac{F\,a_1 a_2}{F\left(a_1 + a_2\right)}a = \dfrac{a_1 a_2}{a_1 + a_2}
Answera = \dfrac{a_1 a_2}{a_1 + a_2}
Problem #37
Dynamics: forces and balanceOn a sled with a load of mass 50\,\text{кг} horizontal force acts 40\,\text{Н}. With what acceleration does the sled move if the coefficient of friction is equal to 0{,}02?
Show the walkthroughHide the walkthrough
- m
- 50\,\text{кг}
- F
- 40\,\text{Н}
- \mu
- 0{,}02
a - ?
- F_{\text{тр}} = \mu m gF_{\text{тр}} = 0{,}02\cdot 50\cdot 10F_{\text{тр}} = 10\,\text{Н}
- F - F_{\text{тр}} = ma\ \Rightarrow\ a = \dfrac{F - F_{\text{тр}}}{m}a = \dfrac{40 - 10}{50}a = 0{,}6\,\tfrac{\text{м}}{\text{с}^{2}}
Answera = 0{,}6\,\tfrac{\text{м}}{\text{с}^{2}}
Problem #38
Dynamics: Newton's lawsForce 4\,\text{Н} imparts acceleration to the body 1{,}25\,\text{м/с}^{2}. What force will impart acceleration to this body? 3\,\text{м/с}^{2}?
Show the walkthroughHide the walkthrough
- F_1
- 4\,\text{Н}
- a_1
- 1{,}25\,\tfrac{\text{м}}{\text{с}^{2}}
- a_2
- 3\,\tfrac{\text{м}}{\text{с}^{2}}
F_2 - ?
- F_1 = ma_1\ \Rightarrow\ m = \dfrac{F_1}{a_1}m = \dfrac{4\,\text{Н}}{1{,}25\,\tfrac{\text{м}}{\text{с}^{2}}}m = 3{,}2\,\text{кг}
- F_2 = ma_2F_2 = 3{,}2\,\text{кг}\cdot 3\,\tfrac{\text{м}}{\text{с}^{2}}F_2 = 9{,}6\,\text{Н}
In short: F_1/F_2 = a_1/a_2, whence F_2 = F_1 a_2 / a_1.
AnswerF_2 = 9{,}6\,\text{Н}
Problem #39
Dynamics: Newton's lawsWith what acceleration does a rocket with a mass of 200\,\text{кг}, if the engine thrust is equal to 3\,\text{кН}?
Show the walkthroughHide the walkthrough
- m
- 200\,\text{кг}
- F_{\text{т}}
- 3\,\text{кН}=3000\,\text{Н}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
a - ?
- F_{\text{т}} - mg = ma\ \Rightarrow\ a = \dfrac{F_{\text{т}} - mg}{m}
Upward is the force of gravity, downward is the force of gravity.
- a = \dfrac{F_{\text{т}} - mg}{m}a = \dfrac{3000 - 200\cdot 10}{200}a = 5\,\tfrac{\text{м}}{\text{с}^{2}}
Answera = 5\,\tfrac{\text{м}}{\text{с}^{2}}
Problem #40
Dynamics: forces and balanceWith what force do the Earth and the Sun attract? Accept M_{\text{З}}=6\cdot10^{24}\,\text{кг}, M_{\text{С}}=2\cdot10^{30}\,\text{кг}, r=1{,}5\cdot10^{11}\,\text{м}. What diameter would a steel cable hold the Earth at its breaking point? 500\cdot10^{6}\,\text{Па}?
Show the walkthroughHide the walkthrough
- M_{\text{З}}
- 6\cdot 10^{24}\,\text{кг}
- M_{\text{С}}
- 2\cdot 10^{30}\,\text{кг}
- r
- 150\cdot 10^{6}\,\text{км}=150\cdot 10^{9}\,\text{м}
- G
- 6{,}67\cdot 10^{-11}\,\tfrac{\text{Н}\cdot\text{м}^{2}}{\text{кг}^{2}}
- \sigma_{\text{пр}}
- 500\cdot 10^{6}\,\text{Па}
F - ?d - ?
- F = G\dfrac{M_{\text{З}}M_{\text{С}}}{r^{2}}F = \dfrac{6{,}67\cdot 10^{-11}\cdot 6\cdot 10^{24}\cdot 2\cdot 10^{30}}{\left(150\cdot 10^{9}\right)^{2}}F = 3{,}56\cdot 10^{22}\,\text{Н}
- \sigma_{\text{пр}} = \dfrac{F}{S}\ \Rightarrow\ S = \dfrac{F}{\sigma_{\text{пр}}}S = \dfrac{3{,}56\cdot 10^{22}}{500\cdot 10^{6}}S = 7{,}1\cdot 10^{13}\,\text{м}^{2}
- S = \dfrac{\pi d^{2}}{4}\ \Rightarrow\ d = \sqrt{\dfrac{4S}{\pi}}d = \sqrt{\dfrac{4\cdot 7{,}1\cdot 10^{13}}{3{,}14}}d = 9{,}5\cdot 10^{6}\,\text{м} = 9500\,\text{км}
AnswerF = 3{,}56\cdot 10^{22}\,\text{Н}d = 9{,}5\cdot 10^{6}\,\text{м}
Problem #41
Dynamics: forces and balancePer body weight 6\,\text{кг} A horizontal force acts on a horizontal table. Take the coefficients of static and sliding friction to be equal 0{,}2. Find the force for uniform sliding and acceleration 1{,}5\,\text{м/с}^{2}. Then find the acceleration of the initially stationary body at forces 5\,\text{Н} and 15\,\text{Н}.
Show the walkthroughHide the walkthrough
- m
- 6\,\text{кг}
- \mu
- 0{,}2
- a
- 1{,}5\,\tfrac{\text{м}}{\text{с}^{2}}
- F'
- 5\,\text{Н}
- F''
- 15\,\text{Н}
F_1 - ?F_2 - ?a' - ?a'' - ?
- F_{\text{тр}} = \mu m gF_{\text{тр}} = 0{,}2\cdot 6\cdot 10F_1 = 12\,\text{Н}
- F_1 = F_{\text{тр}}F_1 = 12\,\text{Н}
For uniform movement, traction balances friction.
- F_2 = F_{\text{тр}} + maF_2 = 12 + 6\cdot 1{,}5F_2 = 21\,\text{Н}
- F' = 5\,\text{Н} < F_{\text{тр}}a' = 0
The body will not move: a static friction force of 5 N arises.
- a'' = \dfrac{F'' - F_{\text{тр}}}{m}a'' = \dfrac{15 - 12}{6}a'' = 0{,}5\,\tfrac{\text{м}}{\text{с}^{2}}
AnswerF_1 = 12\,\text{Н}F_2 = 21\,\text{Н}a' = 0a'' = 0{,}5\,\tfrac{\text{м}}{\text{с}^{2}}
Problem #42
Dynamics: forces and balanceMasses of weights are suspended from the ends of a weightless lever 4\,\text{кг} and 24\,\text{кг}. Distance from fulcrum to smaller load 60\,\text{см}. Determine the length of the lever.
Show the walkthroughHide the walkthrough
- m_1
- 4\,\text{кг}
- m_2
- 24\,\text{кг}
- \ell_1
- 60\,\text{см}
\ell - ?
- m_1 g\,\ell_1 = m_2 g\,\ell_2
Rule of moments about the fulcrum.
- \ell_2 = \dfrac{m_1\ell_1}{m_2}\ell_2 = \dfrac{4\cdot 60}{24}\ell_2 = 10\,\text{см}
- \ell = \ell_1 + \ell_2\ell = 60 + 10\ell = 70\,\text{см}
Answer\ell = 70\,\text{см}
Problem #43
Dynamics: forces and balanceHomogeneous beam of mass 600\,\text{кг} lies on two supports. One support is located at the end of the beam, the other at a distance of a quarter of the length from the other end. With what force does the beam press on the supports?
Show the walkthroughHide the walkthrough
- m
- 600\,\text{кг}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
F_{\text{д}1} - ?F_{\text{д}2} - ?
- mg\cdot\dfrac{L}{2} = N_2\cdot\dfrac{3L}{4}
We take the moments relative to the first support; the center of gravity is in the middle of the beam.
- N_2 = \dfrac{mg\cdot 4}{2\cdot 3} = \dfrac{2mg}{3}N_2 = \dfrac{2\cdot 600\cdot 10}{3}F_{\text{д}2} = 4000\,\text{Н}
- N_1 + N_2 = mg\ \Rightarrow\ N_1 = mg - N_2N_1 = 6000 - 4000F_{\text{д}1} = 2000\,\text{Н}
- F_{\text{д}1} = N_1,\quad F_{\text{д}2} = N_2F_{\text{д}1} = 2000\,\text{Н}\ \text{и}\ 4000\,\text{Н}
According to Newton's third law, the beam presses on the supports with the same forces.
AnswerF_{\text{д}1} = 2000\,\text{Н}F_{\text{д}2} = 4000\,\text{Н}
Problem #44
Dynamics: Newton's lawsMan of mass 80\,\text{кг} presses on the floor of the elevator with force 700\,\text{Н}. Determine the magnitude and direction of acceleration of the elevator.
Show the walkthroughHide the walkthrough
- m
- 80\,\text{кг}
- F_{\text{д}}
- 700\,\text{Н}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
a - ?
- F_{\text{д}} < mg\quad\left(700 < 800\right)\vec{a}\ \text{направлено вниз}
A person presses less than he weighs, which means the elevator accelerates down or slows down when ascending.
- N = F_{\text{д}} = 700\,\text{Н}
According to Newton's third law.
- mg - N = ma\ \Rightarrow\ a = \dfrac{mg - N}{m}a = \dfrac{80\cdot 10 - 700}{80}a = 1{,}25\,\tfrac{\text{м}}{\text{с}^{2}}
Answera = 1{,}25\,\tfrac{\text{м}}{\text{с}^{2}}\ \text{вниз}
Problem #45
Dynamics: forces and balanceUnder the influence of horizontal force 12\,\text{Н} block of mass 5\,\text{кг} moving with acceleration 2\,\text{м/с}^{2}. Determine the coefficient of friction.
Show the walkthroughHide the walkthrough
- F
- 12\,\text{Н}
- m
- 5\,\text{кг}
- a
- 2\,\tfrac{\text{м}}{\text{с}^{2}}
\mu - ?
- F - F_{\text{тр}} = ma\ \Rightarrow\ F_{\text{тр}} = F - maF_{\text{тр}} = 12 - 5\cdot 2F_{\text{тр}} = 2\,\text{Н}
- F_{\text{тр}} = \mu m g\ \Rightarrow\ \mu = \dfrac{F_{\text{тр}}}{mg}\mu = \dfrac{2}{5\cdot 10}\mu = 0{,}04
In one line: mu = (F - ma)/(mg).
Answer\mu = 0{,}04
Problem #46
Dynamics: forces and balanceBody mass 5\,\text{кг} falls from a height 20\,\text{м} for 2{,}1\,\text{с}. Determine the force of air resistance. Accept g=9{,}81\,\text{м/с}^{2}. The body is released without initial velocity; In this model, consider the resistance force to be constant.
Show the walkthroughHide the walkthrough
- m
- 5\,\text{кг}
- h
- 20\,\text{м}
- t
- 2{,}1\,\text{с}
- g
- 9{,}81\,\tfrac{\text{м}}{\text{с}^{2}}
F_{\text{с}} - ?
- h = \dfrac{at^{2}}{2}\ \Rightarrow\ a = \dfrac{2h}{t^{2}}a = \dfrac{2\cdot 20}{2{,}1^{2}}a = 9{,}07\,\tfrac{\text{м}}{\text{с}^{2}}
The actual acceleration is less than g, which means that the air is slowing down the body.
- mg - F_{\text{с}} = ma\ \Rightarrow\ F_{\text{с}} = m\left(g - a\right)5\left(9{,}81 - 9{,}07\right)F_{\text{с}} = 3{,}7\,\text{Н}
AnswerF_{\text{с}} = 3{,}7\,\text{Н}
Problem #47
Dynamics: Newton's lawsForce 6\,\text{Н} imparts acceleration to the body 0{,}4\,\text{м/с}^{2}. What force will impart acceleration to this body? 5\,\text{м/с}^{2}?
Show the walkthroughHide the walkthrough
- F_1
- 6\,\text{Н}
- a_1
- 0{,}4\,\tfrac{\text{м}}{\text{с}^{2}}
- a_2
- 5\,\tfrac{\text{м}}{\text{с}^{2}}
F_2 - ?
- \dfrac{F_1}{F_2} = \dfrac{a_1}{a_2}\ \Rightarrow\ F_2 = \dfrac{F_1 a_2}{a_1}F_2 = \dfrac{6\cdot 5}{0{,}4}F_2 = 75\,\text{Н}
The mass of the body is the same, so the force is proportional to the acceleration.
AnswerF_2 = 75\,\text{Н}
Problem #48
Dynamics: forces and balanceBody mass 2\,\text{кг} slides on a horizontal surface. A horizontal force acts along its velocity 5\,\text{Н}. The sliding friction coefficient is equal to 0{,}4. Find the projection of acceleration onto the direction of velocity before the body stops.
Show the walkthroughHide the walkthrough
- m
- 2\,\text{кг}
- F
- 5\,\text{Н}
- \mu
- 0{,}4
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
a_x - ?
- F - F_{\text{тр}} = ma_x\ \Rightarrow\ a_x = \dfrac{F - \mu m g}{m}\dfrac{5 - 0{,}4\cdot 2\cdot 10}{2} = \dfrac{5 - 8}{2}a_x = -1{,}5\,\tfrac{\text{м}}{\text{с}^{2}}
- F < F_{\text{тр}}\ \Rightarrow\ a_x < 0
The object is already sliding. The net force opposes its velocity, so it slows to a stop. The negative acceleration component describes this slowing down.
Answera_x = -1{,}5\,\tfrac{\text{м}}{\text{с}^{2}}
Problem #49
Dynamics: forces and balanceWhat should be the coefficient of friction so that a motorcyclist can pass a turn with a radius 50\,\text{м} at speed 36\,\text{км/ч}?
Show the walkthroughHide the walkthrough
- R
- 50\,\text{м}
- v
- 36\,\text{км/ч}=10\,\text{м/с}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
\mu - ?
- F_{\text{тр}} = \dfrac{mv^{2}}{R}
During a turn, friction plays the role of centripetal force.
- \mu m g = \dfrac{mv^{2}}{R}\ \Rightarrow\ \mu = \dfrac{v^{2}}{gR}\mu = \dfrac{10^{2}}{10\cdot 50}\mu = 0{,}2
The mass is reduced - the result does not depend on it.
Answer\mu = 0{,}2
Problem #50
Dynamics: Newton's lawsMan of mass 50\,\text{кг} presses on the floor of the elevator with force 600\,\text{Н}. Determine the projection of the elevator's acceleration onto the vertical axis directed upward.
Show the walkthroughHide the walkthrough
- m
- 50\,\text{кг}
- F_{\text{д}}
- 600\,\text{Н}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
a - ?
- F_{\text{д}} > mg\quad\left(600 > 500\right)\vec{a}\ \text{направлено вверх}
- N = F_{\text{д}};\quad N - mg = ma\ \Rightarrow\ a = \dfrac{N - mg}{m}a = \dfrac{600 - 50\cdot 10}{50}a = 2\,\tfrac{\text{м}}{\text{с}^{2}}
Answera = 2\,\tfrac{\text{м}}{\text{с}^{2}}
Problem #51
Dynamics: forces and balanceAt what speed should a cyclist travel so that at the top point of the bridge the radius of curvature 45\,\text{м} push on the bridge with a force half that of gravity?
Show the walkthroughHide the walkthrough
- R
- 45\,\text{м}
- F_{\text{д}}
- \dfrac{mg}{2}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
v - ?
- N = F_{\text{д}} = \dfrac{mg}{2}
At the top point of the bridge, the force of gravity and the reaction of the support are in opposite directions.
- mg - N = ma_{\text{цс}},\quad a_{\text{цс}} = \dfrac{v^{2}}{R}
- mg - \dfrac{mg}{2} = \dfrac{mv^{2}}{R}\ \Rightarrow\ v = \sqrt{R\left(g - \dfrac{g}{2}\right)}\sqrt{45\left(10 - 5\right)} = \sqrt{225}v = 15\,\tfrac{\text{м}}{\text{с}} = 54\,\tfrac{\text{км}}{\text{ч}}
Answerv = 15\,\tfrac{\text{м}}{\text{с}}
Problem #52
Dynamics: forces and balanceWhat is the force holding the car's mass 1200\,\text{кг} at a turn with a radius 250\,\text{м} at speed 90\,\text{км/ч}? What is the maximum speed at the coefficient of friction 0{,}5?
Show the walkthroughHide the walkthrough
- m
- 1200\,\text{кг}
- R
- 250\,\text{м}
- v
- 90\,\text{км/ч}=25\,\text{м/с}
- \mu
- 0{,}5
F - ?v_{\max} - ?
- F = \dfrac{mv^{2}}{R}F = \dfrac{1200\cdot 25^{2}}{250}F = 3000\,\text{Н}
- \mu m g = \dfrac{mv_{\max}^{2}}{R}\ \Rightarrow\ v_{\max} = \sqrt{\mu g R}\sqrt{0{,}5\cdot 10\cdot 250} = \sqrt{1250}v_{\max} = 35{,}4\,\tfrac{\text{м}}{\text{с}}
AnswerF = 3000\,\text{Н}v_{\max} = 35{,}4\,\tfrac{\text{м}}{\text{с}}
Problem #53
Dynamics: Newton's lawsThe elevator is moving with acceleration 2\,\text{м/с}^{2}. The weight presses on the floor with force 2880\,\text{Н}. What two masses of a load are possible depending on the direction of acceleration?
Show the walkthroughHide the walkthrough
- a
- 2\,\tfrac{\text{м}}{\text{с}^{2}}
- F_{\text{д}}
- 2880\,\text{Н}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
m_1 - ?m_2 - ?
- N = F_{\text{д}};\quad N - mg = ma_x\ \Rightarrow\ N = m\left(g + a_x\right)
The sign of acceleration depends on where the elevator is accelerating.
- m_1 = \dfrac{N}{g + a}m_1 = \dfrac{2880}{10 + 2}m_1 = 240\,\text{кг}
Acceleration is directed upward - overload, more weight.
- m_2 = \dfrac{N}{g - a}m_2 = \dfrac{2880}{10 - 2}m_2 = 360\,\text{кг}
Acceleration is directed downwards - partial weightlessness.
Answerm_1 = 240\,\text{кг}m_2 = 360\,\text{кг}
Problem #62
Dynamics: forces and balanceBall mass 500\,\text{г} hanging on a long thread 80\,\text{см}. He is taken to 90^{\circ} and let go. Determine the thread tension at the lowest point.
Show the walkthroughHide the walkthrough
- m
- 500\,\text{г}=0{,}5\,\text{кг}
- R = \ell
- 80\,\text{см}=0{,}8\,\text{м}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
T - ?
- mgh = \dfrac{mv^{2}}{2}\ \Rightarrow\ v = \sqrt{2gh}v = \sqrt{2\cdot 10\cdot 0{,}8}v = 4\,\tfrac{\text{м}}{\text{с}}
The ball is retracted 90°, so it descends exactly the length of the thread.
- T - mg = \dfrac{mv^{2}}{R}\ \Rightarrow\ T = m\left(g + \dfrac{v^{2}}{R}\right)0{,}5\left(10 + \dfrac{4^{2}}{0{,}8}\right)T = 15\,\text{Н}
AnswerT = 15\,\text{Н}
Problem #147
Newton's lawsResultant force on a body of mass 4 kg is equal to 12 H. Find the acceleration.
Show the walkthroughHide the walkthrough
- m
- 4\,\text{кг}
- F
- 12\,\text{Н}
a - ?
- a=\frac{F}{m}a=\frac{12}{4}a=3\,\text{м/с}^{2}
We divide the resultant force, not the individual force, by the mass.
Answer3\,\text{м/с}^{2}
Problem #148
Newton's lawsResultant force on a body of mass 5 kg is equal to 20 H. Find the acceleration.
Show the walkthroughHide the walkthrough
- m
- 5\,\text{кг}
- F
- 20\,\text{Н}
a - ?
- a=\frac{F}{m}a=\frac{20}{5}a=4\,\text{м/с}^{2}
We divide the resultant force, not the individual force, by the mass.
Answer4\,\text{м/с}^{2}
Problem #149
Newton's lawsBody mass 3 kg is pulled to the right by force 20 N, the resistance force to the left is 5 H. Find the acceleration module.
Show the walkthroughHide the walkthrough
- m
- 3\,\text{кг}
- F_1
- 20\,\text{Н}
- F_2
- 5\,\text{Н}
a - ?
- F=F_1-F_2F=20 - 5F=15\,\text{Н}
We choose the positive direction to the right.
- a=\frac{F}{m}a=\frac{15}{3}a=5\,\text{м/с}^{2}
We apply Newton's law to the resultant.
Answer5\,\text{м/с}^{2}
Problem #150
Newton's lawsBody mass 4 kg is pulled to the right by force 30 N, the resistance force to the left is 6 H. Find the acceleration module.
Show the walkthroughHide the walkthrough
- m
- 4\,\text{кг}
- F_1
- 30\,\text{Н}
- F_2
- 6\,\text{Н}
a - ?
- F=F_1-F_2F=30 - 6F=24\,\text{Н}
We choose the positive direction to the right.
- a=\frac{F}{m}a=\frac{24}{4}a=6\,\text{м/с}^{2}
We apply Newton's law to the resultant.
Answer6\,\text{м/с}^{2}
Problem #151
Newton's lawsBody mass 2 kg was at rest. A constant horizontal force was applied to it 14 N at constant resistance force 4 N. Find a way behind 4 s.
Show the walkthroughHide the walkthrough
- m
- 2\,\text{кг}
- F
- 14\,\text{Н}
- R
- 4\,\text{Н}
- t
- 4\,\text{с}
S - ?
- F_{\text{рез}}=F-RF_{\text{рез}}=14 - 4F_{\text{рез}}=10\,\text{Н}
Subtract the opposing force.
- a=\frac{F_{\text{рез}}}{m}a=\frac{10}{2}a=5\,\text{м/с}^{2}
Mass relates force and acceleration.
- S=\frac{at^2}{2}S=\frac{5 \cdot {4}^{2}}{2}S=40\,\text{м}
The initial speed is zero, the acceleration is constant.
Answer40\,\text{м}
Problem #152
Newton's lawsBody mass 3 kg was at rest. A constant horizontal force was applied to it 21 N at constant resistance force 9 N. Find a way behind 5 s.
Show the walkthroughHide the walkthrough
- m
- 3\,\text{кг}
- F
- 21\,\text{Н}
- R
- 9\,\text{Н}
- t
- 5\,\text{с}
S - ?
- F_{\text{рез}}=F-RF_{\text{рез}}=21 - 9F_{\text{рез}}=12\,\text{Н}
Subtract the opposing force.
- a=\frac{F_{\text{рез}}}{m}a=\frac{12}{3}a=4\,\text{м/с}^{2}
Mass relates force and acceleration.
- S=\frac{at^2}{2}S=\frac{4 \cdot {5}^{2}}{2}S=50\,\text{м}
The initial speed is zero, the acceleration is constant.
Answer50\,\text{м}
Problem #153
Forces and equilibriumBody mass 4 kg slides horizontally. Friction coefficient 0{,}2, g = 10 m/s². Find the friction force if there are no other vertical forces.
Show the walkthroughHide the walkthrough
- m
- 4\,\text{кг}
- u
- 0{,}2\,\text{безразм.}
- g
- 10\,\text{м/с}^{2}
F_{\text{тр}} - ?
- F_{\text{тр}}=\mu mgF_{\text{тр}}=0{,}2 \cdot 4 \cdot 10F_{\text{тр}}=8\,\text{Н}
The normal reaction is mg.
Answer8\,\text{Н}
Problem #154
Forces and equilibriumBody mass 6 kg slides horizontally. Friction coefficient 0{,}3, g = 10 m/s². Find the friction force if there are no other vertical forces.
Show the walkthroughHide the walkthrough
- m
- 6\,\text{кг}
- u
- 0{,}3\,\text{безразм.}
- g
- 10\,\text{м/с}^{2}
F_{\text{тр}} - ?
- F_{\text{тр}}=\mu mgF_{\text{тр}}=0{,}3 \cdot 6 \cdot 10F_{\text{тр}}=18\,\text{Н}
The normal reaction is mg.
Answer18\,\text{Н}
Problem #155
Forces and equilibriumThe elevator accelerates up with acceleration 2 m/s². Passenger weight 60 kg, g = 10 m/s². Find the weight of the passenger.
Show the walkthroughHide the walkthrough
- a
- 2\,\text{м/с}^{2}
- m
- 60\,\text{кг}
- g
- 10\,\text{м/с}^{2}
P - ?
- F=maF=60 \cdot 2F=120\,\text{Н}
The resultant is directed upward.
- P=mg+maP=60 \cdot 10 + 120P=720\,\text{Н}
The support reaction exceeds the force of gravity by ma.
Answer720\,\text{Н}
Problem #156
Forces and equilibriumThe elevator accelerates up with acceleration 3 m/s². Passenger weight 70 kg, g = 10 m/s². Find the weight of the passenger.
Show the walkthroughHide the walkthrough
- a
- 3\,\text{м/с}^{2}
- m
- 70\,\text{кг}
- g
- 10\,\text{м/с}^{2}
P - ?
- F=maF=70 \cdot 3F=210\,\text{Н}
The resultant is directed upward.
- P=mg+maP=70 \cdot 10 + 210P=910\,\text{Н}
The support reaction exceeds the force of gravity by ma.
Answer910\,\text{Н}
Problem #157
Forces and equilibriumSpring stiffness 200 N/m stretched by 0{,}1 m and pulls horizontally on a block of mass 2 kg, sliding in the direction of the spring force. The friction coefficient is 0{,}2, g = 10 m/s². Find the acceleration at this moment.
Show the walkthroughHide the walkthrough
- k
- 200\,\text{Н/м}
- x
- 0{,}1\,\text{м}
- m
- 2\,\text{кг}
- u
- 0{,}2\,\text{безразм.}
- g
- 10\,\text{м/с}^{2}
a - ?
- F=kxF=200 \cdot 0{,}1F=20\,\text{Н}
The elastic force at the moment under consideration.
- R=\mu mgR=0{,}2 \cdot 2 \cdot 10R=4\,\text{Н}
Friction is directed against sliding.
- a=\frac{F-R}{m}a=\frac{(20 - 4)}{2}a=8\,\text{м/с}^{2}
We find the instantaneous acceleration using the resultant.
Answer8\,\text{м/с}^{2}
Problem #158
Forces and equilibriumSpring stiffness 300 N/m stretched by 0{,}12 m and pulls horizontally on a block of mass 3 kg, sliding in the direction of the spring force. The friction coefficient is 0{,}2, g = 10 m/s². Find the acceleration at this moment.
Show the walkthroughHide the walkthrough
- k
- 300\,\text{Н/м}
- x
- 0{,}12\,\text{м}
- m
- 3\,\text{кг}
- u
- 0{,}2\,\text{безразм.}
- g
- 10\,\text{м/с}^{2}
a - ?
- F=kxF=300 \cdot 0{,}12F=36\,\text{Н}
The elastic force at the moment under consideration.
- R=\mu mgR=0{,}2 \cdot 3 \cdot 10R=6\,\text{Н}
Friction is directed against sliding.
- a=\frac{F-R}{m}a=\frac{(36 - 6)}{3}a=10\,\text{м/с}^{2}
We find the instantaneous acceleration using the resultant.
Answer10\,\text{м/с}^{2}
The theory behind these problems
Work through the topic if a problem will not give in.
Formulas by topic
Look up symbols and units of measurement in the reference.