Mechanics

227 soru

Soru 141Soru

A body of mass 2.5 kg2.5\text{ kg} moving at a speed of 4.0 m s14.0\text{ m s}^{-1} along a straight horizontal path is brought to rest in 2.0 s2.0\text{ s} by a constant retarding force. What is the magnitude of this retarding force in newtons?

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Cevap: 5

Cevap

The magnitude of the retarding force is 5.0 N5.0\text{ N}.
According to Newton's second law of motion, net force is equal to the rate of change of momentum (F=ΔpΔt=m(vu)tF = \frac{\Delta p}{\Delta t} = \frac{m(v-u)}{t}). Substituting m=2.5 kgm = 2.5\text{ kg}, u=4.0 m s1u = 4.0\text{ m s}^{-1}, v=0 m s1v = 0\text{ m s}^{-1}, and t=2.0 st = 2.0\text{ s} gives F=2.5×(04.0)2.0=5.0 NF = \frac{2.5 \times (0 - 4.0)}{2.0} = -5.0\text{ N}. The magnitude of this force is 5.0 N5.0\text{ N}.

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1
Determine the initial momentum and final momentum of the body.
Initial momentum pi=2.5×4.0=10.0 kg m s1p_i = 2.5 \times 4.0 = 10.0\text{ kg m s}^{-1}, and final momentum pf=0 kg m s1p_f = 0\text{ kg m s}^{-1}.
Linear momentum is defined as the product of mass and velocity (p=mvp = mv).
2
Calculate the magnitude of the force applied using the impulse-momentum relationship F=ΔpΔtF = \frac{\Delta p}{\Delta t}.
Magnitude of force F=010.02.0=5.0 NF = \frac{|0 - 10.0|}{2.0} = 5.0\text{ N}.
Newton's second law states that the rate of change of momentum is equal to the net external force applied.

Anahtar Kavram

Newton's Second Law and Impulse-Momentum Relationship
Tahmini Süre:45s
Soru 142Soru

A constant horizontal force of 25 N25\text{ N} is applied to push a box across a smooth horizontal surface through a displacement of 8 m8\text{ m} in the direction of the force. What is the total work done on the box?

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Cevap: 200 J200\text{ J}

Cevap

The work done on the box is 200 J200\text{ J}.
Work done is defined as the product of force and distance moved in the direction of the force (W=F×dW = F \times d). Substituting the given values F=25 NF = 25\text{ N} and d=8 md = 8\text{ m} gives W=200 JW = 200\text{ J}.

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1
Identify the given physical quantities
Force F=25 NF = 25\text{ N}, displacement d=8 md = 8\text{ m}, angle θ=0\theta = 0^\circ
Work depends on force and displacement along the line of action
2
Apply the work formula W=Fdcos(θ)W = F \cdot d \cos(\theta)
W=25 N×8 m×cos(0)=200 JW = 25\text{ N} \times 8\text{ m} \times \cos(0^\circ) = 200\text{ J}
Since force and displacement are in the same direction, cos(0)=1\cos(0^\circ) = 1

Anahtar Kavram

Work Done by a Constant Force
Soru 143Soru

A body of mass 3.0 kg3.0\text{ kg} moving due east along a smooth horizontal track at 8.0 m s18.0\text{ m s}^{-1} collides head-on with a 2.0 kg2.0\text{ kg} body moving due west at 4.0 m s14.0\text{ m s}^{-1}. Immediately after the impact, the 2.0 kg2.0\text{ kg} body rebounds due east with a speed of 5.0 m s15.0\text{ m s}^{-1}. If the duration of the impact is 0.02 s0.02\text{ s}, what is the magnitude of the average impact force exerted on the 3.0 kg3.0\text{ kg} body?

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Cevap: 900 N900\text{ N}

Cevap

The magnitude of the average impact force exerted on the 3.0 kg3.0\text{ kg} body is 900 N900\text{ N}.
By designating East as positive, initial velocities are u1=+8.0 m s1u_1 = +8.0\text{ m s}^{-1} and u2=4.0 m s1u_2 = -4.0\text{ m s}^{-1}. Conservation of linear momentum gives (3.0×8.0)+(2.0×4.0)=3.0v1+(2.0×5.0)(3.0 \times 8.0) + (2.0 \times -4.0) = 3.0 v_1 + (2.0 \times 5.0), yielding v1=+2.0 m s1v_1 = +2.0\text{ m s}^{-1}. The change in momentum of the 3.0 kg3.0\text{ kg} body is Δp=3.0×(2.08.0)=18.0 N s\Delta p = 3.0 \times (2.0 - 8.0) = -18.0\text{ N s}. Dividing the magnitude of this impulse by the impact time (0.02 s0.02\text{ s}) yields an average force of 900 N900\text{ N}.

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1
Set up momentum conservation by assigning directional signs to velocities.
Taking East as positive (++): u1=+8.0 m s1u_1 = +8.0\text{ m s}^{-1}, u2=4.0 m s1u_2 = -4.0\text{ m s}^{-1}, v2=+5.0 m s1v_2 = +5.0\text{ m s}^{-1}.
Linear momentum is a vector quantity, so direction must be taken into account.
2
Calculate the initial total momentum and solve for the final velocity of the 3.0 kg3.0\text{ kg} body (v1v_1).
m1u1+m2u2=m1v1+m2v2    (3.0×8.0)+(2.0×4.0)=3.0v1+(2.0×5.0)    16.0=3.0v1+10.0    v1=+2.0 m s1m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2 \implies (3.0 \times 8.0) + (2.0 \times -4.0) = 3.0 v_1 + (2.0 \times 5.0) \implies 16.0 = 3.0 v_1 + 10.0 \implies v_1 = +2.0\text{ m s}^{-1}.
Total momentum is conserved in the absence of external forces.
3
Calculate the magnitude of the impulse and average force acting on the 3.0 kg3.0\text{ kg} body.
Δp1=m1(v1u1)=3.0×(2.08.0)=18.0 N s\Delta p_1 = m_1(v_1 - u_1) = 3.0 \times (2.0 - 8.0) = -18.0\text{ N s}. Force magnitude F=Δp1Δt=18.00.02=900 NF = \frac{|\Delta p_1|}{\Delta t} = \frac{18.0}{0.02} = 900\text{ N}.
The average force equals the rate of change of linear momentum.

Anahtar Kavram

Law of Conservation of Linear Momentum and Impulse-Momentum Theorem
Tahmini Süre:2m 0s
Soru 144Soru

An electric train traveling along a straight track uniformly slows down from a speed of 30 m/s30\text{ m/s} to 10 m/s10\text{ m/s} over a distance of 200 m200\text{ m}. What is the magnitude of the deceleration of the train in m/s2\text{m/s}^2?

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Cevap: 2

Cevap

The magnitude of the deceleration is 2 m/s22\text{ m/s}^2.
Using the kinematic equation v2=u2+2asv^2 = u^2 + 2as, substituting v=10 m/sv = 10\text{ m/s}, u=30 m/su = 30\text{ m/s}, and s=200 ms = 200\text{ m} gives 100=900+400a100 = 900 + 400a, which simplifies to 400a=800400a = -800, yielding a=2 m/s2a = -2\text{ m/s}^2. The magnitude of deceleration is 2 m/s22\text{ m/s}^2.

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1
Identify the given kinematic variables.
Initial velocity u=30 m/su = 30\text{ m/s}, final velocity v=10 m/sv = 10\text{ m/s}, displacement s=200 ms = 200\text{ m}.
Choosing the appropriate equation of motion requires knowing which variables are given and which is unknown.
2
Apply the third equation of motion relating initial velocity, final velocity, acceleration, and distance.
v2=u2+2asv^2 = u^2 + 2as
This formula connects uu, vv, aa, and ss without needing time tt.
3
Substitute the given values into the equation and solve for acceleration aa.
(10)2=(30)2+2(a)(200)    100=900+400a    400a=800    a=2 m/s2(10)^2 = (30)^2 + 2(a)(200) \implies 100 = 900 + 400a \implies 400a = -800 \implies a = -2\text{ m/s}^2.
Performing algebraic operations to isolate the acceleration parameter.
4
State the magnitude of the deceleration.
The magnitude of deceleration is 2 m/s22\text{ m/s}^2.
Deceleration represents the rate of speed reduction, which corresponds to the magnitude of negative acceleration.

Anahtar Kavram

Uniformly Accelerated Motion Equations
Soru 145Soru

Car AA, traveling at a constant speed of 20 m/s20\text{ m/s} along a straight horizontal road, passes a landmark 50 m50\text{ m} ahead of car BB, which is initially stationary. At t=0 st = 0\text{ s}, car BB starts moving in the same direction, accelerating uniformly at 3.0 m/s23.0\text{ m/s}^2 until it reaches a top speed of 30 m/s30\text{ m/s}, after which it continues at this constant top speed. How many seconds after t=0 st = 0\text{ s} does car BB catch up with car AA?

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Cevap: 20

Cevap

Car B catches up with car A after 20 seconds.
Car B accelerates for 10 s10\text{ s} covering 150 m150\text{ m} to reach 30 m/s30\text{ m/s}. During these 10 s10\text{ s}, car A reaches a position of 250 m250\text{ m} (taking into account its 50 m50\text{ m} head start). Car B then closes the remaining 100 m100\text{ m} gap at a relative speed of 10 m/s10\text{ m/s} (30 m/s20 m/s30\text{ m/s} - 20\text{ m/s}), taking an extra 10 s10\text{ s}. The total elapsed time is 10 s+10 s=20 s10\text{ s} + 10\text{ s} = 20\text{ s}.

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1
Calculate the duration t1t_1 of car B's acceleration phase to reach 30 m/s30\text{ m/s}.
t1=vmaxua=3003.0=10 st_1 = \frac{v_{max} - u}{a} = \frac{30 - 0}{3.0} = 10\text{ s}
Car B accelerates uniformly from rest at 3.0 m/s23.0\text{ m/s}^2 until reaching its top speed limit.
2
Determine the distance sBs_B covered by car B and the position sAs_A of car A at t=10 st = 10\text{ s}.
sB=12at12=12(3.0)(10)2=150 ms_B = \frac{1}{2}a t_1^2 = \frac{1}{2}(3.0)(10)^2 = 150\text{ m}; sA=50+vAt1=50+(20)(10)=250 ms_A = 50 + v_A t_1 = 50 + (20)(10) = 250\text{ m}
Car A starts 50 m50\text{ m} ahead and moves continuously at 20 m/s20\text{ m/s}.
3
Find the separation distance between the two cars at t=10 st = 10\text{ s} and compute the time Δt\Delta t required to close it.
\text{Separation} = 250 - 150 = 100\text{ m}; \Delta t = \frac{100}{30 - 20} = 10\text{ s}
Beyond t=10 st = 10\text{ s}, car B travels at a constant relative velocity of 10 m/s10\text{ m/s} faster than car A.
4
Sum the acceleration time and constant speed time to find the total time taken.
ttotal=t1+Δt=10 s+10 s=20 st_{total} = t_1 + \Delta t = 10\text{ s} + 10\text{ s} = 20\text{ s}
Combining both phases yields the exact instant car B overtakes car A.

Anahtar Kavram

Multi-stage relative motion with acceleration limits
Soru 146Soru

A solid block floats in water of density 1000 kg/m31000\text{ kg/m}^3 with 60%60\% of its total volume submerged. When the same block is placed in an unknown liquid XX, 80%80\% of its total volume is submerged. What is the density of liquid XX?

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Cevap: 750 kg/m3750\text{ kg/m}^3

Cevap

The density of liquid XX is 750 kg/m3750\text{ kg/m}^3.
For any floating body, its weight equals the upthrust exerted by the liquid. The upthrust is given by U=ρfluidVsubmergedgU = \rho_{\text{fluid}} \cdot V_{\text{submerged}} \cdot g. Since the weight of the block is unchanged, ρwaterVsub, water=ρXVsub, X\rho_{\text{water}} \cdot V_{\text{sub, water}} = \rho_X \cdot V_{\text{sub, X}}. Substituting the given values: 1000×0.60V=ρX×0.80V1000 \times 0.60V = \rho_X \times 0.80V, yielding ρX=750 kg/m3\rho_X = 750\text{ kg/m}^3.

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1
Apply the Law of Flotation to the block in water
Weight of block W=ρwVsub, waterg=10000.60Vg=600VgW = \rho_w \cdot V_{\text{sub, water}} \cdot g = 1000 \cdot 0.60V \cdot g = 600 V g
A floating object displaces its own weight of fluid.
2
Apply the Law of Flotation to the block in liquid X
Weight of block W=ρXVsub, Xg=ρX0.80VgW = \rho_X \cdot V_{\text{sub, X}} \cdot g = \rho_X \cdot 0.80V \cdot g
The weight of the block remains constant regardless of the fluid.
3
Equate the two expressions for the weight of the block and solve for ρX\rho_X
ρX0.80Vg=600Vg    ρX=6000.80=750 kg/m3\rho_X \cdot 0.80V \cdot g = 600 V g \implies \rho_X = \frac{600}{0.80} = 750\text{ kg/m}^3
Since both buoyant forces equal the block's weight, set them equal to each other.

Anahtar Kavram

Law of Flotation and Archimedes' Principle
Soru 147Soru

A solid object has a mass of 0.50 kg0.50\text{ kg} and a volume of 2.0×104 m32.0 \times 10^{-4}\text{ m}^3. If it is completely immersed in a liquid of density 800 kg/m3800\text{ kg/m}^3, what is the magnitude of the upthrust exerted on the object? [Take g=10 m/s2g = 10\text{ m/s}^2]

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Cevap: 1.6 N1.6\text{ N}

Cevap

The magnitude of the upthrust exerted on the object is 1.6 N1.6\text{ N}.
By Archimedes' Principle, upthrust is equal to the weight of the liquid displaced: U=ρliquidVgU = \rho_{\text{liquid}} V g. Substituting ρ=800 kg/m3\rho = 800\text{ kg/m}^3, V=2.0×104 m3V = 2.0 \times 10^{-4}\text{ m}^3, and g=10 m/s2g = 10\text{ m/s}^2 yields 1.6 N1.6\text{ N}.

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1
Identify the given values and state Archimedes' Principle
Volume of displaced liquid V=2.0×104 m3V = 2.0 \times 10^{-4}\text{ m}^3, density of liquid ρ=800 kg/m3\rho = 800\text{ kg/m}^3, acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2. Upthrust formula is U=ρVgU = \rho V g.
According to Archimedes' Principle, the upward buoyant force (upthrust) equals the weight of the liquid displaced by the submerged object.
2
Calculate the upthrust
U=800 kg/m3×(2.0×104 m3)×10 m/s2=1.6 NU = 800\text{ kg/m}^3 \times (2.0 \times 10^{-4}\text{ m}^3) \times 10\text{ m/s}^2 = 1.6\text{ N}.
Multiplying fluid density by submerged volume and gravitational acceleration gives the force in newtons.

Anahtar Kavram

Archimedes' Principle and Upthrust
Soru 148Soru

A spherical ball bearing of radius 3.0 mm3.0\text{ mm} and density 5400 kg/m35400\text{ kg/m}^3 falls vertically through a viscous oil of density 900 kg/m3900\text{ kg/m}^3 and dynamic viscosity coefficient 0.10 Pas0.10\text{ Pa}\cdot\text{s}. Assuming the motion obeys Stokes' law and taking the acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the terminal velocity of the sphere?

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Cevap: 0.90 m/s0.90\text{ m/s}

Cevap

The terminal velocity of the sphere is 0.90 m/s0.90\text{ m/s}.
At terminal velocity, the downward force of gravity (weight of the sphere) is balanced by the sum of two upward forces: the buoyant force (upthrust) and the viscous drag force given by Stokes' law (Fv=6πηrvTF_v = 6\pi \eta r v_T). Using the formula vT=2r2(ρsρf)g9ηv_T = \frac{2 r^2 (\rho_s - \rho_f) g}{9 \eta} with r=3.0×103 mr = 3.0 \times 10^{-3}\text{ m}, ρsρf=4500 kg/m3\rho_s - \rho_f = 4500\text{ kg/m}^3, η=0.10 Pas\eta = 0.10\text{ Pa}\cdot\text{s}, and g=10 m/s2g = 10\text{ m/s}^2 yields 0.90 m/s0.90\text{ m/s}.

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1
Convert given parameters to standard SI units
Radius r=3.0 mm=3.0×103 mr = 3.0\text{ mm} = 3.0 \times 10^{-3}\text{ m}, density of sphere ρs=5400 kg/m3\rho_s = 5400\text{ kg/m}^3, density of liquid ρf=900 kg/m3\rho_f = 900\text{ kg/m}^3, viscosity η=0.10 Pas\eta = 0.10\text{ Pa}\cdot\text{s}, g=10 m/s2g = 10\text{ m/s}^2.
Ensures dimensional consistency across all terms in the physical equations.
2
Apply the equilibrium condition at terminal velocity
At terminal velocity vTv_T, downward weight equals upward forces: W=U+FvW = U + F_v, where W=43πr3ρsgW = \frac{4}{3}\pi r^3 \rho_s g, U=43πr3ρfgU = \frac{4}{3}\pi r^3 \rho_f g, and Fv=6πηrvTF_v = 6\pi \eta r v_T.
Terminal velocity is reached when net acceleration is zero.
3
Rearrange Stokes' law formula for terminal velocity
vT=2r2(ρsρf)g9ηv_T = \frac{2 r^2 (\rho_s - \rho_f) g}{9 \eta}
Isolates the target unknown variable vTv_T.
4
Substitute the physical values and solve
vT=2×(3.0×103)2×(5400900)×109×0.10=2×(9.0×106)×4500×100.90=0.810.90=0.90 m/sv_T = \frac{2 \times (3.0 \times 10^{-3})^2 \times (5400 - 900) \times 10}{9 \times 0.10} = \frac{2 \times (9.0 \times 10^{-6}) \times 4500 \times 10}{0.90} = \frac{0.81}{0.90} = 0.90\text{ m/s}.
Calculates the final quantitative answer.

Anahtar Kavram

Viscosity and Stokes' Law for terminal velocity of a sphere in a viscous fluid
Tahmini Süre:2m 0s
Soru 149Soru

A simple pendulum of length LL and bob mass mm has a period of oscillation TT on the surface of the Earth. The length of the pendulum is increased by 44%44\%, its bob mass is doubled to 2m2m, and the entire apparatus is transported to a planet where the acceleration due to gravity is 36%36\% less than that on Earth. What is the new period of oscillation of the pendulum?

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Cevap: 1.5T1.5T

Cevap

1.5T1.5T
The period of a simple pendulum is determined by T=2πLgT = 2\pi \sqrt{\frac{L}{g}}. It is entirely independent of the mass of the bob. With a length increase of 44%44\% (L=1.44LL' = 1.44L) and a gravity reduction of 36%36\% (g=0.64gg' = 0.64g), the new period becomes 1.440.64T=1.20.8T=1.5T\sqrt{\frac{1.44}{0.64}}T = \frac{1.2}{0.8}T = 1.5T.

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1
State the equation for the period of a simple pendulum
T=2πLgT = 2\pi \sqrt{\frac{L}{g}}
The period depends solely on length LL and acceleration due to gravity gg, and is independent of mass mm.
2
Determine the new length and new acceleration due to gravity
L=1.44LL' = 1.44L and g=0.64gg' = 0.64g
A 44%44\% increase in length yields 1+0.44=1.441 + 0.44 = 1.44, while a 36%36\% decrease in gravity yields 10.36=0.641 - 0.36 = 0.64.
3
Calculate the factor of change in the period
TT=LL×gg=1.440.64=14464=128=1.5\frac{T'}{T} = \sqrt{\frac{L'}{L} \times \frac{g}{g'}} = \sqrt{\frac{1.44}{0.64}} = \sqrt{\frac{144}{64}} = \frac{12}{8} = 1.5
Substituting the relative changes into the pendulum period ratio yields the scaling factor.
4
Express the new period in terms of TT
T=1.5TT' = 1.5T
Multiplying the initial period by the calculated scaling factor gives the final period.

Anahtar Kavram

Mass independence and parametric scaling of simple pendulum period in Simple Harmonic Motion
Soru 150Soru

A solid sphere of mass 0.60 kg0.60\text{ kg} and volume 2.0×104 m32.0 \times 10^{-4}\text{ m}^3 is released from rest in a tall vessel filled with a viscous liquid of density 1000 kg/m31000\text{ kg/m}^3. As the sphere falls, it eventually reaches a constant terminal velocity of 4.0 m/s4.0\text{ m/s}. Assuming that the viscous drag force is directly proportional to the speed of the sphere, what is the magnitude of the viscous drag force acting on the sphere when its speed is 1.5 m/s1.5\text{ m/s}? (Take g=10 m/s2g = 10\text{ m/s}^2)

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Cevap: 1.50 N1.50\text{ N}

Cevap

1.50 N1.50\text{ N}
At terminal velocity, the sphere is in translational equilibrium under three forces: downward weight (6.0 N6.0\text{ N}), upward upthrust (2.0 N2.0\text{ N}), and upward viscous drag (4.0 N4.0\text{ N}). Since viscous drag is directly proportional to velocity (Fv=kvF_v = k v), the proportionality constant kk is 1.0 Ns/m1.0\text{ N}\cdot\text{s/m}. Therefore, at 1.5 m/s1.5\text{ m/s}, the viscous force is 1.0×1.5=1.50 N1.0 \times 1.5 = 1.50\text{ N}.

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1
Calculate the downward gravitational force (weight) acting on the sphere.
W=m×g=0.60 kg×10 m/s2=6.0 NW = m \times g = 0.60\text{ kg} \times 10\text{ m/s}^2 = 6.0\text{ N}
Weight is the force pulling the sphere downward.
2
Calculate the buoyant force (upthrust) exerted by the liquid using Archimedes' principle.
U=ρl×V×g=1000 kg/m3×(2.0×104 m3)×10 m/s2=2.0 NU = \rho_l \times V \times g = 1000\text{ kg/m}^3 \times (2.0 \times 10^{-4}\text{ m}^3) \times 10\text{ m/s}^2 = 2.0\text{ N}
Upthrust equals the weight of the fluid displaced by the submerged sphere.
3
Determine the viscous drag force at terminal velocity (vt=4.0 m/sv_t = 4.0\text{ m/s}) using equilibrium of forces.
Fv(vt)=WU=6.0 N2.0 N=4.0 NF_v(v_t) = W - U = 6.0\text{ N} - 2.0\text{ N} = 4.0\text{ N}
At terminal velocity, the net acceleration is zero, so downward weight is balanced by upward upthrust and viscous drag.
4
Find the constant of proportionality kk for viscous drag (Fv=kvF_v = k v).
k=Fv(vt)vt=4.0 N4.0 m/s=1.0 Ns/mk = \frac{F_v(v_t)}{v_t} = \frac{4.0\text{ N}}{4.0\text{ m/s}} = 1.0\text{ N}\cdot\text{s/m}
Viscous force is given as directly proportional to speed.
5
Calculate the viscous drag force at a speed of 1.5 m/s1.5\text{ m/s}.
Fv(1.5)=k×1.5 m/s=1.0 Ns/m×1.5 m/s=1.50 NF_v(1.5) = k \times 1.5\text{ m/s} = 1.0\text{ N}\cdot\text{s/m} \times 1.5\text{ m/s} = 1.50\text{ N}
Applying the constant kk to the specified speed.

Anahtar Kavram

Terminal velocity in viscous fluids and Archimedes' Principle
Tahmini Süre:2m 30s
Soru 151Soru

A non-uniform wooden pole of length 6.0 m6.0\text{ m} and weight 150 N150\text{ N} is balanced horizontally on a pivot placed 2.4 m2.4\text{ m} from its heavy end PP. The system achieves rotational equilibrium when a load of 50 N50\text{ N} is hung directly from end PP. What is the distance of the center of gravity of the pole from end PP?

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Cevap: 3.2

Cevap

The distance of the center of gravity of the pole from end PP is 3.2 m3.2\text{ m}.
Taking moments about the pivot at 2.4 m2.4\text{ m} from end PP, the counter-clockwise moment created by the 50 N50\text{ N} load (50 N×2.4 m=120 Nm50\text{ N} \times 2.4\text{ m} = 120\text{ N}\cdot\text{m}) must balance the clockwise moment created by the 150 N150\text{ N} weight of the pole acting at its center of gravity (150 N×(d2.4 m)150\text{ N} \times (d - 2.4\text{ m})). Equating these gives 120=150(d2.4)120 = 150(d - 2.4), leading to d2.4=0.8 md - 2.4 = 0.8\text{ m}, so d=3.2 md = 3.2\text{ m}.

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1
Identify force positions relative to the pivot
The 50 N50\text{ N} load is 2.4 m2.4\text{ m} to the left of the pivot. The 150 N150\text{ N} weight acts at the center of gravity, which is (d2.4 m)(d - 2.4\text{ m}) to the right of the pivot.
Moments are evaluated relative to the fulcrum to eliminate the unknown normal reaction force at the pivot.
2
Apply the Principle of Moments
Anti-clockwise moment = 50×2.4=120 Nm50 \times 2.4 = 120\text{ N}\cdot\text{m}. Clockwise moment = 150×(d2.4)150 \times (d - 2.4). Setting them equal: 120=150(d2.4)120 = 150(d - 2.4).
For a body in rotational equilibrium, the total clockwise moment about any pivot equals the total anti-clockwise moment.
3
Solve the equation for distance dd
d2.4=0.8    d=3.2 md - 2.4 = 0.8 \implies d = 3.2\text{ m}.
Adding the displacement from the pivot (0.8 m0.8\text{ m}) to the pivot position from end PP (2.4 m2.4\text{ m}) yields the position of the center of gravity from end PP.

Anahtar Kavram

Rotational equilibrium and Principle of Moments for non-uniform rigid bodies
Tahmini Süre:1m 30s
Soru 152Soru

A particle of mass 0.50 kg0.50\text{ kg} executes simple harmonic motion along a straight line. When its displacement from the equilibrium position is 0.06 m0.06\text{ m}, its speed is 0.80 m/s0.80\text{ m/s} and its potential energy is 0.09 J0.09\text{ J}. What is the magnitude of the maximum acceleration of the particle in m/s2\text{m/s}^2?

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Cevap: 10

Cevap

The magnitude of the maximum acceleration of the particle is 10 m/s210\text{ m/s}^2.
Using potential energy Ep=12mω2x2E_p = \frac{1}{2}m\omega^2 x^2, the angular frequency ω\omega is 10 rad/s10\text{ rad/s}. Using v=ωA2x2v = \omega\sqrt{A^2 - x^2}, the amplitude AA is 0.10 m0.10\text{ m}. Substituting these values into amax=ω2Aa_{\max} = \omega^2 A yields 10 m/s210\text{ m/s}^2.

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1
Find angular frequency ω\omega from potential energy.
ω=10 rad/s\omega = 10\text{ rad/s}
Using potential energy Ep=12mω2x2E_p = \frac{1}{2}m\omega^2 x^2: 0.09=12(0.50)ω2(0.06)2    0.09=0.0009ω2    ω2=100    ω=10 rad/s0.09 = \frac{1}{2}(0.50)\omega^2 (0.06)^2 \implies 0.09 = 0.0009 \omega^2 \implies \omega^2 = 100 \implies \omega = 10\text{ rad/s}.
2
Find amplitude AA from speed.
A=0.10 mA = 0.10\text{ m}
Using speed v=ωA2x2v = \omega\sqrt{A^2 - x^2}: 0.80=10A20.062    0.08=A20.0036    0.0064=A20.0036    A2=0.0100    A=0.10 m0.80 = 10\sqrt{A^2 - 0.06^2} \implies 0.08 = \sqrt{A^2 - 0.0036} \implies 0.0064 = A^2 - 0.0036 \implies A^2 = 0.0100 \implies A = 0.10\text{ m}.
3
Calculate maximum acceleration.
amax=10 m/s2a_{\max} = 10\text{ m/s}^2
Using maximum acceleration formula amax=ω2Aa_{\max} = \omega^2 A: amax=100×0.10=10 m/s2a_{\max} = 100 \times 0.10 = 10\text{ m/s}^2.

Anahtar Kavram

Simple Harmonic Motion Energy and Kinematic Relations
Soru 153Soru

A solid alloy specimen weighs 240 g240\text{ g} in air, 180 g180\text{ g} when completely immersed in water, and 195 g195\text{ g} when completely immersed in an unknown liquid XX. What is the relative density of liquid XX?

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Cevap: 0.750.75

Cevap

The relative density of liquid X is 0.750.75.
According to Archimedes' principle, relative density of a liquid is the ratio of the upthrust experienced by a solid in that liquid to the upthrust experienced by the same solid in water. Upthrust in water is 240 g180 g=60 g240\text{ g} - 180\text{ g} = 60\text{ g}, and upthrust in liquid X is 240 g195 g=45 g240\text{ g} - 195\text{ g} = 45\text{ g}. Dividing 4545 by 6060 gives 0.750.75.

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1
Calculate the upthrust in water
240 g180 g=60 g240\text{ g} - 180\text{ g} = 60\text{ g}
By Archimedes' principle, upthrust in water equals the mass loss when immersed in water.
2
Calculate the upthrust in liquid X
240 g195 g=45 g240\text{ g} - 195\text{ g} = 45\text{ g}
Upthrust in liquid X equals the mass loss when immersed in liquid X.
3
Determine the relative density of liquid X
\text{Relative Density} = \frac{\text{Upthrust in liquid X}}{\text{Upthrust in water}} = \frac{45\text{ g}}{60\text{ g}} = 0.75
Relative density of a liquid is defined as the ratio of the weight of a given volume of the liquid to the weight of an equal volume of water.

Anahtar Kavram

Archimedes' Principle and Relative Density of Liquids
Tahmini Süre:1m 30s
Soru 154Soru

A 0.40 kg0.40\text{ kg} mass attached to a light helical spring undergoes simple harmonic motion on a smooth horizontal surface. If the force constant of the spring is 160 N/m160\text{ N/m} and the amplitude of oscillation is 0.05 m0.05\text{ m}, what is the maximum speed of the mass?

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Cevap: 1.0 m/s1.0\text{ m/s}

Cevap

The maximum speed of the mass is 1.0 m/s1.0\text{ m/s}.
The angular frequency of the mass-spring system is calculated using \(\omega = \sqrt{k/m} = \sqrt{160/0.40} = 20\text{ rad/s}\). Multiplying this by the amplitude \(A = 0.05\text{ m}\) yields a maximum speed of \(v_{\text{max}} = 1.0\text{ m/s}\).

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1
Calculate the angular frequency (\(\omega\)) of the mass-spring system.
\(\omega = \sqrt{\frac{k}{m}} = \sqrt{\frac{160\text{ N/m}}{0.40\text{ kg}}} = \sqrt{400} = 20\text{ rad/s}\)
The angular frequency of a spring-mass oscillator depends on the spring constant and the mass.
2
Determine the maximum speed (\(v_{\text{max}}\)) using the amplitude.
\(v_{\text{max}} = \omega A = 20\text{ rad/s} \times 0.05\text{ m} = 1.0\text{ m/s}\)
In simple harmonic motion, maximum speed occurs at the equilibrium position and equals the product of angular frequency and amplitude.

Anahtar Kavram

Maximum velocity in simple harmonic motion for a mass-spring system
Soru 155Soru

A solid block of wood has a mass of 0.60 kg0.60\text{ kg}. When placed in a vessel of water, it floats freely on the surface. What is the magnitude of the upthrust exerted by the water on the block? (Take g=10 m/s2g = 10\text{ m/s}^2)

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Cevap: 6.0 N6.0\text{ N}

Cevap

The upthrust exerted by the water on the floating block is 6.0 N6.0\text{ N}.
According to the Law of Flotation, a body floating freely in a fluid displaces a weight of fluid equal to its own weight. Therefore, the upward force (upthrust) exerted by the fluid is equal to the weight of the block: U=mg=0.60 kg×10 m/s2=6.0 NU = mg = 0.60\text{ kg} \times 10\text{ m/s}^2 = 6.0\text{ N}.

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1
Determine the weight of the floating block in air.
W=mg=0.60 kg×10 m/s2=6.0 NW = mg = 0.60\text{ kg} \times 10\text{ m/s}^2 = 6.0\text{ N}
Weight is the force of gravity acting on the block's mass.
2
Apply the Law of Flotation to find the upthrust.
Upthrust U=W=6.0 NU = W = 6.0\text{ N}
A freely floating body displaces a volume of fluid whose weight is equal to the total weight of the body.

Anahtar Kavram

Law of Flotation and Archimedes' Principle
Tahmini Süre:45s
Soru 156Soru

A solid wooden block of density 600 kg/m3600\text{ kg/m}^3 and volume 4.0×103 m34.0 \times 10^{-3}\text{ m}^3 floats in water of density 1000 kg/m31000\text{ kg/m}^3. A metal block is placed on top of the wooden block so that the wooden block is just completely submerged while the metal block remains entirely above the water surface. What is the mass of the metal block? (Take g=10 m/s2g = 10\text{ m/s}^2)

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Cevap: 1.6 kg1.6\text{ kg}

Cevap

1.6 kg1.6\text{ kg}
When the wooden block is completely submerged, it displaces 4.0×103 m34.0 \times 10^{-3}\text{ m}^3 of water, creating an upthrust of 40 N40\text{ N}. The weight of the wooden block is 24 N24\text{ N}. For equilibrium, the total downward weight must equal the upthrust (24 N+Wmetal=40 N24\text{ N} + W_{\text{metal}} = 40\text{ N}), which gives Wmetal=16 NW_{\text{metal}} = 16\text{ N} and a corresponding mass of 1.6 kg1.6\text{ kg}.

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1
Calculate the mass and weight of the wooden block.
mwood=ρwood×Vwood=600 kg/m3×4.0×103 m3=2.4 kgm_{\text{wood}} = \rho_{\text{wood}} \times V_{\text{wood}} = 600\text{ kg/m}^3 \times 4.0 \times 10^{-3}\text{ m}^3 = 2.4\text{ kg}, so Wwood=2.4×10=24 NW_{\text{wood}} = 2.4 \times 10 = 24\text{ N}.
The weight of the wood contributes to the total downward force of the floating system.
2
Calculate the total upthrust exerted by the water when the wooden block is completely submerged.
U=ρwater×Vwood×g=1000 kg/m3×4.0×103 m3×10 m/s2=40 NU = \rho_{\text{water}} \times V_{\text{wood}} \times g = 1000\text{ kg/m}^3 \times 4.0 \times 10^{-3}\text{ m}^3 \times 10\text{ m/s}^2 = 40\text{ N}.
By Archimedes' principle, upthrust equals the weight of the displaced liquid.
3
Apply the law of flotation to solve for the weight and mass of the metal block.
Wwood+Wmetal=U    24 N+Wmetal=40 N    Wmetal=16 NW_{\text{wood}} + W_{\text{metal}} = U \implies 24\text{ N} + W_{\text{metal}} = 40\text{ N} \implies W_{\text{metal}} = 16\text{ N}. Thus, mmetal=16 N10 m/s2=1.6 kgm_{\text{metal}} = \frac{16\text{ N}}{10\text{ m/s}^2} = 1.6\text{ kg}.
For the system to float in equilibrium just submerged, total downward weight must equal total upward buoyant force.

Anahtar Kavram

Archimedes' Principle and Law of Flotation
Tahmini Süre:2m 0s
Soru 157Soru

A vertical light spring stretches by 0.10 m0.10\text{ m} when a block is suspended from it in equilibrium. The block is then pulled down an additional 0.05 m0.05\text{ m} from its equilibrium position and released from rest to undergo simple harmonic motion. Taking acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the speed of the block when it is at a displacement of 0.03 m0.03\text{ m} from its equilibrium position?

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Cevap: 0.40 m/s0.40\text{ m/s}

Cevap

0.40 m/s0.40\text{ m/s}
The system's angular frequency ω\omega is determined by the equilibrium extension ee using ω=ge=10 rad/s\omega = \sqrt{\frac{g}{e}} = 10\text{ rad/s}. Combining this with the amplitude A=0.05 mA = 0.05\text{ m} in the SHM speed relation v=ωA2y2v = \omega \sqrt{A^2 - y^2} at y=0.03 my = 0.03\text{ m} yields v=10(0.05)2(0.03)2=0.40 m/sv = 10 \sqrt{(0.05)^2 - (0.03)^2} = 0.40\text{ m/s}.

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1
Calculate the angular frequency of the mass-spring system using static equilibrium conditions.
ω=10 rad/s\omega = 10\text{ rad/s}
At equilibrium, mg=ke    km=gemg = ke \implies \frac{k}{m} = \frac{g}{e}. Therefore, ω=ge=100.10=10 rad/s\omega = \sqrt{\frac{g}{e}} = \sqrt{\frac{10}{0.10}} = 10\text{ rad/s}.
2
Identify the amplitude of simple harmonic motion.
A=0.05 mA = 0.05\text{ m}
The initial displacement from the equilibrium position when released from rest defines the amplitude of oscillation.
3
Apply the SHM velocity-displacement formula v=ωA2y2v = \omega \sqrt{A^2 - y^2} at y=0.03 my = 0.03\text{ m}.
v=0.40 m/sv = 0.40\text{ m/s}
v=10×(0.05)2(0.03)2=10×0.00250.0009=10×0.04=0.40 m/sv = 10 \times \sqrt{(0.05)^2 - (0.03)^2} = 10 \times \sqrt{0.0025 - 0.0009} = 10 \times 0.04 = 0.40\text{ m/s}.

Anahtar Kavram

Relating static extension to angular frequency and calculating instantaneous speed in Simple Harmonic Motion
Soru 158Soru

A particle of mass 0.20 kg0.20\text{ kg} executes simple harmonic motion along a straight line. When its displacement from the equilibrium position is 0.03 m0.03\text{ m}, its speed is 0.16 m/s0.16\text{ m/s}. When its displacement is 0.04 m0.04\text{ m}, its speed is 0.12 m/s0.12\text{ m/s}. What is the total mechanical energy of the particle in millijoules (mJ\text{mJ})?

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Cevap: 4

Cevap

The total mechanical energy of the particle is 4 mJ4\text{ mJ}.
Using the relation v2=ω2(A2x2)v^2 = \omega^2(A^2 - x^2) for the two given state points (0.03 m,0.16 m/s)(0.03\text{ m}, 0.16\text{ m/s}) and (0.04 m,0.12 m/s)(0.04\text{ m}, 0.12\text{ m/s}) forms a set of simultaneous equations. Subtracting them yields ω2=16 rad2/s2\omega^2 = 16\text{ rad}^2/\text{s}^2, leading to A2=0.0025 m2A^2 = 0.0025\text{ m}^2. Substituting these values into E=12mω2A2E = \frac{1}{2}m\omega^2 A^2 gives E=0.004 JE = 0.004\text{ J}, which converts to 4 mJ4\text{ mJ}.

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1
Set up kinematic equations for both displacement points using v2=ω2(A2x2)v^2 = \omega^2(A^2 - x^2).
0.0256=ω2(A20.0009)0.0256 = \omega^2(A^2 - 0.0009) and 0.0144=ω2(A20.0016)0.0144 = \omega^2(A^2 - 0.0016).
The equation relates linear speed, angular frequency, amplitude, and instantaneous displacement in SHM.
2
Subtract the two simultaneous equations to eliminate A2A^2 and find ω2\omega^2.
0.0112=0.0007ω2    ω2=16 rad2/s20.0112 = 0.0007\omega^2 \implies \omega^2 = 16\text{ rad}^2/\text{s}^2.
Eliminating amplitude isolates the angular frequency squared.
3
Determine A2A^2 by substituting ω2=16\omega^2 = 16 back into one of the state equations.
A2=0.0025 m2    A=0.05 mA^2 = 0.0025\text{ m}^2 \implies A = 0.05\text{ m}.
Amplitude is required to calculate the maximum potential or total mechanical energy.
4
Calculate total mechanical energy E=12mω2A2E = \frac{1}{2}m\omega^2 A^2 and convert to millijoules.
E=12×0.20×16×0.0025=0.004 J=4 mJE = \frac{1}{2} \times 0.20 \times 16 \times 0.0025 = 0.004\text{ J} = 4\text{ mJ}.
Total energy in SHM is constant and proportional to mass, square of angular frequency, and square of amplitude.

Anahtar Kavram

Conservation of energy and phase-space relationship between velocity and displacement in simple harmonic motion.
Soru 159Soru

A small spherical lead shot of radius 3.0×103 m3.0 \times 10^{-3}\text{ m} and density 8000 kg/m38000\text{ kg/m}^3 falls vertically through a viscous oil of density 800 kg/m3800\text{ kg/m}^3 and dynamic viscosity 0.18 Pas0.18\text{ Pa}\cdot\text{s}. What is the magnitude of the terminal velocity of the sphere in m/s\text{m/s}? (Take g=10 m/s2g = 10\text{ m/s}^2)

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Cevap: 0.8

Cevap

The terminal velocity of the lead shot is 0.8 m/s0.8\text{ m/s}.
At terminal velocity, acceleration is zero because the upward forces (viscous drag 6πηrvt6\pi \eta r v_t plus buoyant upthrust 43πr3ρfg\frac{4}{3}\pi r^3 \rho_f g) completely balance the downward weight of the sphere (43πr3ρsg\frac{4}{3}\pi r^3 \rho_s g). Solving for velocity gives vt=2r2(ρsρf)g9η=0.8 m/sv_t = \frac{2 r^2 (\rho_s - \rho_f) g}{9 \eta} = 0.8\text{ m/s}.

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1
Formulate the force balance equation at terminal velocity.
Weight (WW) = Upthrust (UU) + Viscous drag (FvF_v), which simplifies to vt=2r2(ρsρf)g9ηv_t = \frac{2 r^2 (\rho_s - \rho_f) g}{9 \eta}.
When terminal velocity is attained, the net acceleration of the sphere is zero, so upward forces balance downward force.
2
Substitute the physical parameters into the terminal velocity formula.
vt=2×(3.0×103)2×(8000800)×109×0.18=0.8 m/sv_t = \frac{2 \times (3.0 \times 10^{-3})^2 \times (8000 - 800) \times 10}{9 \times 0.18} = 0.8\text{ m/s}.
Direct calculation using Stokes' law and Archimedes' principle.

Anahtar Kavram

Terminal Velocity and Stokes' Law in a Viscous Medium
Soru 160Soru

A uniform horizontal rod ABAB of length 2.0 m2.0\text{ m} and mass 6.0 kg6.0\text{ kg} is suspended horizontally by two light vertical strings attached at end AA and at a point CC located 0.5 m0.5\text{ m} from end BB. Taking g=10 m/s2g = 10\text{ m/s}^2, what is the tension in the string at point CC in Newtons?

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Cevap: 40

Cevap

The tension in the string at point C is 40 N.
The weight of the rod (60 N60\text{ N}) acts at its midpoint (1.0 m1.0\text{ m} from end AA). Point CC is located 1.5 m1.5\text{ m} from end AA. Taking moments about end AA gives 60 N×1.0 m=TC×1.5 m60\text{ N} \times 1.0\text{ m} = T_C \times 1.5\text{ m}, which evaluates to TC=40 NT_C = 40\text{ N}.

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1
Calculate total weight and identify the center of gravity position
Weight W=60 NW = 60\text{ N} acting at 1.0 m1.0\text{ m} from end AA
For a uniform rod, the weight acts vertically downwards at its geometric center.
2
Set up the moment equilibrium equation taking end A as pivot
60 N×1.0 m=TC×1.5 m60\text{ N} \times 1.0\text{ m} = T_C \times 1.5\text{ m}
Taking moments about point AA eliminates the force at AA and equates clockwise moment from weight to counter-clockwise moment from tension at CC.
3
Solve for the tension force at point C
TC=40 NT_C = 40\text{ N}
Dividing the total moment of 60 Nm60\text{ N}\cdot\text{m} by the moment arm of 1.5 m1.5\text{ m} yields 40 N40\text{ N}.

Anahtar Kavram

Principle of Moments and Rotational Equilibrium
Tahmini Süre:1m 30s
ÖncekiSayfa 8 / 12Sonraki