Mechanics

227 soru

Soru 161Soru

A U-tube open to the atmosphere at both ends contains water of density 1000 kg m31000\text{ kg m}^{-3}. An immiscible liquid is poured into one arm of the tube until it forms a column of height 15.0 cm15.0\text{ cm}. If the interface between the two liquids lies 12.0 cm12.0\text{ cm} below the surface of the water in the opposite arm, what is the density of the liquid in kg m3\text{kg m}^{-3}?

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Cevap: 800

Cevap

The density of the immiscible liquid is 800 kg m3800\text{ kg m}^{-3}.
At the level of the liquid interface, the hydrostatic pressure exerted by the 15.0 cm15.0\text{ cm} liquid column must equal the hydrostatic pressure exerted by the 12.0 cm12.0\text{ cm} water column above it. Equating ρ1h1=ρ2h2\rho_1 h_1 = \rho_2 h_2 yields ρliquid=1000×(12.0/15.0)=800 kg m3\rho_{\text{liquid}} = 1000 \times (12.0 / 15.0) = 800\text{ kg m}^{-3}.

Adım Adım Çözüm

1
Apply the principal of equal pressure at the same horizontal level in a continuous fluid at rest.
Pressure due to liquid column equals pressure due to water column above the interface line.
Hydrostatic pressure at depth hh is given by P=ρghP = \rho g h, and points at equal depth in a connected liquid body share identical pressure.
2
Set up the density-height ratio relationship: ρliquidhliquid=ρwaterhwater\rho_{\text{liquid}} \cdot h_{\text{liquid}} = \rho_{\text{water}} \cdot h_{\text{water}}.
ρliquid=ρwater×hwaterhliquid\rho_{\text{liquid}} = \rho_{\text{water}} \times \frac{h_{\text{water}}}{h_{\text{liquid}}}.
Acceleration due to gravity gg cancels out from both sides of the pressure balance equation.
3
Substitute hliquid=15.0 cmh_{\text{liquid}} = 15.0\text{ cm}, hwater=12.0 cmh_{\text{water}} = 12.0\text{ cm}, and ρwater=1000 kg m3\rho_{\text{water}} = 1000\text{ kg m}^{-3}.
ρliquid=1000×12.015.0=800 kg m3\rho_{\text{liquid}} = 1000 \times \frac{12.0}{15.0} = 800\text{ kg m}^{-3}.
Heights can remain in centimeters since their unit ratio is dimensionless.

Anahtar Kavram

Hydrostatic Pressure Balance in U-Tube Manometers
Tahmini Süre:1m 30s
Soru 162Soru

A uniform beam PQPQ of length 4.0 m4.0\text{ m} and mass 20 kg20\text{ kg} is supported horizontally on a pivot at end PP and by a vertical wire attached at end QQ. A load of mass 30 kg30\text{ kg} is placed on the beam at a distance of 1.0 m1.0\text{ m} from PP. Taking the acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the tension in the vertical wire attached at QQ in newtons?

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Cevap: 175

Cevap

The tension in the vertical wire attached at end QQ is 175 N175\text{ N}.
By applying the principle of moments about the pivot at PP, the sum of downward clockwise moments produced by the 30 kg30\text{ kg} load (300 N×1.0 m=300 Nm300\text{ N} \times 1.0\text{ m} = 300\text{ N}\cdot\text{m}) and the beam's center of gravity (200 N×2.0 m=400 Nm200\text{ N} \times 2.0\text{ m} = 400\text{ N}\cdot\text{m}) equals 700 Nm700\text{ N}\cdot\text{m}. Equating this to the counterclockwise moment of the tension force (T×4.0 mT \times 4.0\text{ m}) gives T=175 NT = 175\text{ N}.

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1
Determine forces and their perpendicular distances from the pivot at PP.
The load exerts a downward force of 300 N300\text{ N} at 1.0 m1.0\text{ m} from PP. The uniform beam's weight of 200 N200\text{ N} acts at its midpoint (2.0 m2.0\text{ m} from PP). The vertical tension TT acts upward at QQ (4.0 m4.0\text{ m} from PP).
Before applying the principle of moments, all force magnitudes and their distance arms relative to the pivot point must be identified.
2
Equate total clockwise moments to total counterclockwise moments about PP.
(300 N×1.0 m)+(200 N×2.0 m)=T×4.0 m(300\text{ N} \times 1.0\text{ m}) + (200\text{ N} \times 2.0\text{ m}) = T \times 4.0\text{ m}
For rotational equilibrium, the sum of clockwise moments about any pivot must equal the sum of counterclockwise moments about that same pivot.
3
Calculate the value of the tension force TT.
T=7004.0=175 NT = \frac{700}{4.0} = 175\text{ N}
Simplifying the moment equation gives the magnitude of the upward supporting force.

Anahtar Kavram

Principle of Moments and Rotational Equilibrium
Soru 163Soru

A light rigid lever of length 2.5 m2.5\text{ m} is pivoted horizontally at one end OO. A downward vertical weight of 60 N60\text{ N} is hung from the lever at a distance of 1.5 m1.5\text{ m} from OO. An upward force FF inclined at an angle of 3030^\circ to the lever is applied at the free end. What is the magnitude of the force FF required to maintain horizontal equilibrium?

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Cevap: 72 N72\text{ N}

Cevap

The magnitude of the force FF required to maintain equilibrium is 72 N72\text{ N}.
According to the Principle of Moments, for a body in rotational equilibrium, the total clockwise moment about a pivot equals the total counterclockwise moment. The load creates a clockwise moment of 60 N×1.5 m=90 Nm60\text{ N} \times 1.5\text{ m} = 90\text{ N}\cdot\text{m}. The force FF applied at 3030^\circ has a perpendicular component of Fsin30=0.5FF \sin 30^\circ = 0.5F. The counterclockwise moment is 0.5F×2.5 m=1.25F0.5F \times 2.5\text{ m} = 1.25F. Setting 1.25F=90 Nm1.25F = 90\text{ N}\cdot\text{m} gives F=72 NF = 72\text{ N}.

Adım Adım Çözüm

1
Calculate the clockwise moment about the pivot OO caused by the hanging load.
Clockwise Moment=60 N×1.5 m=90 Nm\text{Clockwise Moment} = 60\text{ N} \times 1.5\text{ m} = 90\text{ N}\cdot\text{m}
The force of 60 N60\text{ N} acts perpendicularly at a distance of 1.5 m1.5\text{ m} from the pivot.
2
Express the counterclockwise moment about the pivot OO exerted by the force FF.
Counterclockwise Moment=Fsin(30)×2.5 m=1.25F Nm\text{Counterclockwise Moment} = F \sin(30^\circ) \times 2.5\text{ m} = 1.25 F\text{ N}\cdot\text{m}
Only the perpendicular component of the force, Fsin(30)F \sin(30^\circ), contributes to the moment about pivot OO.
3
Equate the clockwise and counterclockwise moments according to the Principle of Moments.
1.25F=90    F=901.25=72 N1.25 F = 90 \implies F = \frac{90}{1.25} = 72\text{ N}
For rotational equilibrium, the sum of clockwise moments must equal the sum of counterclockwise moments.

Anahtar Kavram

Principle of Moments and Perpendicular Force Components
Soru 164Soru

Planet PP has a mean uniform density that is twice that of Planet QQ, and a radius that is half that of Planet QQ. What is the ratio of the escape velocity at the surface of Planet PP to the escape velocity at the surface of Planet QQ?

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Cevap: 12\frac{1}{\sqrt{2}}

Cevap

12\frac{1}{\sqrt{2}}
The correct answer is derived by substituting the planet's mass in terms of radius and density (M=43πR3ρM = \frac{4}{3}\pi R^3 \rho) into the escape velocity equation ve=2GMRv_e = \sqrt{\frac{2GM}{R}}. Simplifying gives ve=R83πGρv_e = R\sqrt{\frac{8}{3}\pi G \rho}, which means escape velocity is proportional to RρR\sqrt{\rho}. Halving the radius and doubling the density yields a factor of 12×2=22=12\frac{1}{2} \times \sqrt{2} = \frac{\sqrt{2}}{2} = \frac{1}{\sqrt{2}}.

Adım Adım Çözüm

1
Express the mass of a uniform spherical planet in terms of its radius RR and density ρ\rho.
M=43πR3ρM = \frac{4}{3}\pi R^3 \rho
Mass equals volume multiplied by mean density.
2
Substitute mass into the escape velocity formula ve=2GMRv_e = \sqrt{\frac{2GM}{R}}.
ve=2G(43πR3ρ)R=R83πGρv_e = \sqrt{\frac{2G \left(\frac{4}{3}\pi R^3 \rho\right)}{R}} = R\sqrt{\frac{8}{3}\pi G \rho}
This establishes the proportionality veRρv_e \propto R\sqrt{\rho}.
3
Set up the ratio of escape velocity for Planet PP to Planet QQ using RP=12RQR_P = \frac{1}{2}R_Q and ρP=2ρQ\rho_P = 2\rho_Q.
\frac{v_{e,P}}{v_{e,Q}} = \frac{R_P\sqrt{\rho_P}}{R_Q\sqrt{\rho_Q}} = \frac{\left(\frac{1}{2}R_Q\right)\sqrt{2\rho_Q}}{R_Q\sqrt{\rho_Q}} = \frac{1}{2}\sqrt{2} = \frac{1}{\sqrt{2}}
Evaluating the ratio of proportional quantities yields the final scale factor.

Anahtar Kavram

Dependence of Escape Velocity on Planet Density and Radius
Tahmini Süre:2m 0s
Soru 165Soru

A satellite revolves around a planet in a circular orbit of radius 1.0×104 km1.0 \times 10^4 \text{ km} with an orbital period of 12 hours12 \text{ hours}. Calculate the orbital period, in hours, of a second satellite orbiting the same planet in a circular path of radius 4.0×104 km4.0 \times 10^4 \text{ km}.

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Cevap: 96

Cevap

96 hours
According to Kepler's Third Law (T2r3T^2 \propto r^3), the orbital period TT scales with radius rr as Tr3/2T \propto r^{3/2}. Increasing the orbital radius by a factor of 4 increases the period by a factor of 43/2=84^{3/2} = 8. Multiplying the original period of 12 hours by 8 yields 96 hours.

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1
Set up Kepler's Third Law equation relating orbital period and orbital radius.
T22T12=r23r13\frac{T_2^2}{T_1^2} = \frac{r_2^3}{r_1^3}
Kepler's Third Law states that the square of the orbital period of a body in circular orbit is directly proportional to the cube of the radius of its orbit.
2
Substitute the given orbital radii and evaluate the scaling factor.
\frac{r_2}{r_1} = \frac{4.0 \times 10^4 \text{ km}}{1.0 \times 10^4 \text{ km}} = 4
Simplifying the ratio of the two orbital radii gives a factor of 4 increase in radius.
3
Calculate the period multiplier by taking the ratio to the power of 3/2.
4^{3/2} = (\sqrt{4})^3 = 2^3 = 8
Taking T2=T1×(r2r1)3/2T_2 = T_1 \times \left(\frac{r_2}{r_1}\right)^{3/2} shows the period scales by a factor of 8.
4
Multiply the initial orbital period by the scaling factor to find the final answer.
T_2 = 12 \text{ hours} \times 8 = 96 \text{ hours}
Multiplying the baseline period of 12 hours by 8 yields the new orbital period.

Anahtar Kavram

Kepler's Third Law of Planetary Motion
Tahmini Süre:1m 30s
Soru 166Soru

A uniform horizontal beam ABAB of length 4.0 m4.0\text{ m} and mass 10 kg10\text{ kg} is hinged smoothly to a vertical wall at end AA. It is held horizontally in static equilibrium by a light cable attached to end BB and anchored to the wall above AA, making an angle of 3030^\circ with the beam. A mass of 5 kg5\text{ kg} is suspended from the beam at a distance of 3.0 m3.0\text{ m} from hinge AA. Taking acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the tension in the cable?

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Cevap: 175 N175\text{ N}

Cevap

The tension in the cable is 175 N175\text{ N}.
Applying the principle of moments about the hinge at end A, the clockwise moments due to the beam's center of mass (100 N100\text{ N} at 2.0 m2.0\text{ m}) and the suspended load (50 N50\text{ N} at 3.0 m3.0\text{ m}) are balanced by the counterclockwise moment of the cable tension (Tsin30T \sin 30^\circ at 4.0 m4.0\text{ m}). Solving (100×2.0)+(50×3.0)=2.0T(100 \times 2.0) + (50 \times 3.0) = 2.0 T yields T=175 NT = 175\text{ N}.

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1
Calculate the downward gravitational forces (weights) acting on the system.
Weight of beam Wbeam=mbeamg=10 kg×10 m/s2=100 NW_{\text{beam}} = m_{\text{beam}} g = 10\text{ kg} \times 10\text{ m/s}^2 = 100\text{ N} acting at 2.0 m2.0\text{ m} from AA. Weight of load Wload=mloadg=5 kg×10 m/s2=50 NW_{\text{load}} = m_{\text{load}} g = 5\text{ kg} \times 10\text{ m/s}^2 = 50\text{ N} acting at 3.0 m3.0\text{ m} from AA.
Forces causing clockwise moments must be expressed in force units (newtons) and located at their respective lines of action.
2
Formulate the equilibrium condition using the Principle of Moments about hinge AA.
\sum \tau_A = 0 \implies (W_{\text{beam}} \times 2.0\text{ m}) + (W_{\text{load}} \times 3.0\text{ m}) = T \sin(30^\circ) \times 4.0\text{ m}
The hinge AA eliminates reaction forces at the hinge from the moment equation.
3
Substitute numerical values and solve for tension TT.
(100 \times 2.0) + (50 \times 3.0) = T \times 0.5 \times 4.0 \implies 200 + 150 = 2.0 T \implies 350 = 2.0 T \implies T = 175\text{ N}$.
Perpendicular distance from AA to line of action of tension is 4.0sin30=2.0 m4.0 \sin 30^\circ = 2.0\text{ m}.

Anahtar Kavram

Equilibrium of rigid bodies and Principle of Moments under non-perpendicular forces
Tahmini Süre:2m 0s
Soru 167Soru

A satellite of mass 500 kg500\text{ kg} orbits a spherical planet of radius R=6.0×106 mR = 6.0 \times 10^6\text{ m} with surface gravitational acceleration g=10 m/s2g = 10\text{ m/s}^2. The satellite is transferred from an initial circular orbit of radius 2R2R to a higher circular orbit of radius 3R3R. What is the minimum energy required, in megajoules (MJ\text{MJ}), to perform this transfer?

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Cevap: 2500

Cevap

The minimum energy required to perform the orbital transfer is 2500 MJ2500\text{ MJ}.
The minimum energy needed to move a satellite between circular orbits is equal to the change in its total mechanical energy (E=GMm2rE = -\frac{GMm}{2r}). Expressing GMGM as gR2gR^2, the energy difference between radii 2R2R and 3R3R simplifies to ΔE=gRm12\Delta E = \frac{gRm}{12}, which evaluates to 2500 MJ2500\text{ MJ}.

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1
Relate surface acceleration due to gravity to planet mass and radius.
GM=gR2GM = gR^2
At the planet's surface (r=Rr = R), gravitational acceleration is g=GMR2g = \frac{GM}{R^2}.
2
Formulate the total mechanical energy equation for a circular orbit.
E=GMm2r=gR2m2rE = -\frac{GMm}{2r} = -\frac{gR^2 m}{2r}
Total energy is kinetic energy GMm2r\frac{GMm}{2r} plus gravitational potential energy GMmr-\frac{GMm}{r}.
3
Calculate initial and final total energies.
E1=gRm4E_1 = -\frac{gRm}{4} and E2=gRm6E_2 = -\frac{gRm}{6}
Substitute the orbit radii r1=2Rr_1 = 2R and r2=3Rr_2 = 3R into the total energy equation.
4
Determine the net work required for the transfer.
ΔE=E2E1=gRm12\Delta E = E_2 - E_1 = \frac{gRm}{12}
The energy required equals the difference in total mechanical energy between the final and initial orbits.
5
Substitute given numerical values and convert joules to megajoules.
ΔE=10×(6.0×106)×50012=2.5×109 J=2500 MJ\Delta E = \frac{10 \times (6.0 \times 10^6) \times 500}{12} = 2.5 \times 10^9\text{ J} = 2500\text{ MJ}
Dividing 2.5×109 J2.5 \times 10^9\text{ J} by 10610^6 converts the value to megajoules.

Anahtar Kavram

Total Mechanical Energy of a Satellite in Circular Orbit and Orbital Transfer Energy
Tahmini Süre:3m 0s
Soru 168Soru

An astronaut has a weight of 720 N720\text{ N} on the surface of the Earth. Calculate the weight of the astronaut, in Newtons (N\text{N}), at an altitude equal to twice the radius of the Earth (h=2Rh = 2R).

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Cevap: 80

Cevap

The weight of the astronaut at an altitude of 2R2R is 80 N80\text{ N}.
At an altitude of 2R2R, the total distance from the center of the Earth is r=R+2R=3Rr = R + 2R = 3R. Because gravitational force follows the inverse-square law (W1/r2W \propto 1/r^2), tripling the distance reduces the gravitational force and weight by a factor of 32=93^2 = 9. Dividing the surface weight of 720 N720\text{ N} by 99 yields 80 N80\text{ N}.

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1
Determine the total distance from the center of the Earth
r=R+2R=3Rr = R + 2R = 3R
Gravitational force depends on the distance measured from the center of mass of the Earth, which is the sum of Earth's radius RR and altitude hh.
2
Apply the inverse-square law of gravitation to find field strength at altitude
g=g32=g9g' = \frac{g}{3^2} = \frac{g}{9}
Acceleration due to gravity is inversely proportional to the square of the distance from the planet's center (g1r2g \propto \frac{1}{r^2}).
3
Calculate the astronaut's weight at altitude
W=7209=80 NW' = \frac{720}{9} = 80\text{ N}
Weight is directly proportional to gravitational field strength (W=mgW = mg).

Anahtar Kavram

Variation of Acceleration due to Gravity with Altitude (Inverse Square Law)
Soru 169Soru

Two point masses of 4.0 kg4.0\text{ kg} and 9.0 kg9.0\text{ kg} are separated by a distance of 5.0 m5.0\text{ m} in free space. At what distance from the 4.0 kg4.0\text{ kg} mass along the line joining them is the net gravitational field strength equal to zero?

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Cevap: 2.0 m2.0\text{ m}

Cevap

The distance from the 4.0 kg4.0\text{ kg} mass where the net gravitational field strength is zero is 2.0 m2.0\text{ m}.
At the point where the net gravitational field strength is zero, the gravitational field intensity produced by the 4.0 kg4.0\text{ kg} mass must equal the intensity produced by the 9.0 kg9.0\text{ kg} mass in magnitude. Equating G(4.0)x2=G(9.0)(5.0x)2\frac{G (4.0)}{x^2} = \frac{G (9.0)}{(5.0 - x)^2} and taking square roots yields 2x=35x\frac{2}{x} = \frac{3}{5 - x}. Cross-multiplying gives 102x=3x10 - 2x = 3x, which yields x=2.0 mx = 2.0\text{ m} from the 4.0 kg4.0\text{ kg} mass.

Adım Adım Çözüm

1
Set up the condition for zero net gravitational field strength.
E1=E2    Gm1x2=Gm2(dx)2E_1 = E_2 \implies \frac{G m_1}{x^2} = \frac{G m_2}{(d - x)^2}
At the neutral point, the opposing gravitational field vectors due to both masses are equal in magnitude.
2
Substitute given values m1=4.0 kgm_1 = 4.0\text{ kg}, m2=9.0 kgm_2 = 9.0\text{ kg}, and total distance d=5.0 md = 5.0\text{ m}.
4.0x2=9.0(5.0x)2\frac{4.0}{x^2} = \frac{9.0}{(5.0 - x)^2}
Simplifying by canceling GG from both sides of the equation.
3
Take the square root of both sides and solve for xx.
\frac{2.0}{x} = \frac{3.0}{5.0 - x} \implies 2.0(5.0 - x) = 3.0x \implies 10.0 - 2.0x = 3.0x \implies 5.0x = 10.0 \implies x = 2.0\text{ m}
Taking the square root simplifies the quadratic relationship into a linear ratio.

Anahtar Kavram

Gravitational Field Strength Neutral Point
Tahmini Süre:1m 0s
Soru 170Soru

A toy car of mass 0.5 kg0.5\text{ kg} moves along a smooth horizontal surface at a constant speed of 4 m s14\text{ m s}^{-1}. What is the kinetic energy of the toy car?

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Cevap: 4 J4\text{ J}

Cevap

The kinetic energy of the toy car is 4 J4\text{ J}.
Substituting the given values into the formula Ek=12mv2E_k = \frac{1}{2} m v^2 gives Ek=12×0.5×42=4 JE_k = \frac{1}{2} \times 0.5 \times 4^2 = 4\text{ J}.

Adım Adım Çözüm

1
Identify the given physical quantities
Mass m=0.5 kgm = 0.5\text{ kg} and speed v=4 m s1v = 4\text{ m s}^{-1}.
These are the mandatory inputs needed to determine kinetic energy.
2
Apply the kinetic energy formula
Ek=12mv2E_k = \frac{1}{2} m v^2
Kinetic energy of a translational body is defined as half the product of its mass and the square of its speed.
3
Substitute the values and compute the result
Ek=12×0.5 kg×(4 m s1)2=0.25×16=4 JE_k = \frac{1}{2} \times 0.5\text{ kg} \times (4\text{ m s}^{-1})^2 = 0.25 \times 16 = 4\text{ J}.
Evaluating the mathematical operation yields the energy in Joules.

Anahtar Kavram

Kinetic Energy
Tahmini Süre:45s
Soru 171Soru

A screw jack with a pitch of 4 mm4\text{ mm} and a tommy bar of length 56 cm56\text{ cm} is used to raise a heavy load of mass 1100 kg1100\text{ kg}. If an effort force of 50 N50\text{ N} is applied at the outer end of the tommy bar, what is the efficiency of the screw jack? (Take π=227\pi = \frac{22}{7} and g=10 m/s2g = 10\text{ m/s}^2)

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Cevap: 25%

Cevap

The efficiency of the screw jack is 25%
The mechanical advantage is calculated as MA=11,000 N50 N=220MA = \frac{11,000\text{ N}}{50\text{ N}} = 220. The velocity ratio for a screw jack is VR=2πRp=2×227×0.56 m0.004 m=880VR = \frac{2 \pi R}{p} = \frac{2 \times \frac{22}{7} \times 0.56\text{ m}}{0.004\text{ m}} = 880. Dividing MAMA by VRVR and multiplying by 100%100\% yields an efficiency of 220880×100%=25%\frac{220}{880} \times 100\% = 25\%.

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1
Calculate the load force (weight) from the given mass.
W=m×g=1100 kg×10 m/s2=11,000 NW = m \times g = 1100\text{ kg} \times 10\text{ m/s}^2 = 11,000\text{ N}
Mass must be converted to weight force in newtons to compute mechanical advantage.
2
Calculate the Mechanical Advantage (MA).
MA=LoadEffort=11,000 N50 N=220MA = \frac{\text{Load}}{\text{Effort}} = \frac{11,000\text{ N}}{50\text{ N}} = 220
Mechanical advantage is the ratio of output load force to input effort force.
3
Calculate the Velocity Ratio (VR) of the screw jack.
VR=2πRp=2×227×0.56 m0.004 m=3.52 m0.004 m=880VR = \frac{2 \pi R}{p} = \frac{2 \times \frac{22}{7} \times 0.56\text{ m}}{0.004\text{ m}} = \frac{3.52\text{ m}}{0.004\text{ m}} = 880
Velocity ratio is the distance moved by the effort in one full revolution (2πR2\pi R) divided by the distance moved by the load in one revolution (pitch pp).
4
Calculate the efficiency of the machine.
Efficiency=MAVR×100%=220880×100%=25%\text{Efficiency} = \frac{MA}{VR} \times 100\% = \frac{220}{880} \times 100\% = 25\%
Efficiency is defined as the ratio of Mechanical Advantage to Velocity Ratio multiplied by 100%.

Anahtar Kavram

Mechanical Advantage, Velocity Ratio, and Efficiency of a Screw Jack
Soru 172Soru

An object undergoing simple harmonic motion completes 2020 complete oscillations in a time duration of 10.0 s10.0\text{ s}. What is the period of oscillation of the object in seconds?

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Cevap: 0.5

Cevap

The period of oscillation is 0.5 s0.5\text{ s}.
The period of simple harmonic motion is the time taken to complete one single oscillation. Dividing the total time (10.0 s10.0\text{ s}) by the number of oscillations (2020) yields 0.5 s0.5\text{ s}.

Adım Adım Çözüm

1
Apply the definition of oscillation period
T=tNT = \frac{t}{N}
Period TT measures the time required for a single complete cycle.
2
Calculate the numerical value for period
T=10.0 s20=0.5 sT = \frac{10.0\text{ s}}{20} = 0.5\text{ s}
Dividing total elapsed time by total completed oscillations gives time per oscillation.

Anahtar Kavram

Period of Simple Harmonic Motion
Soru 173Soru

A conveyor system pulls a 40 kg40\text{ kg} crate at a constant speed of 3 m s13\text{ m s}^{-1} up a rough inclined ramp. The ramp rises 3 m3\text{ m} for every 5 m5\text{ m} measured along its slope (giving sinθ=0.6\sin\theta = 0.6 and cosθ=0.8\cos\theta = 0.8). If the coefficient of kinetic friction between the crate and the ramp is 0.250.25 and g=10 m s2g = 10\text{ m s}^{-2}, what is the power output of the conveyor system in watts?

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Cevap: 960

Cevap

The power output required by the conveyor system is 960 W960\text{ W}.
To pull the crate up the ramp at constant speed, the conveyor force must overcome both the parallel gravitational component (240 N240\text{ N}) and friction (80 N80\text{ N}), making the total force 320 N320\text{ N}. Multiplying this force by the constant speed of 3 m s13\text{ m s}^{-1} gives a total power output of 960 W960\text{ W}.

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1
Calculate the component of weight parallel to the inclined plane
Fg=mgsinθ=40×10×0.6=240 NF_g = mg \sin\theta = 40 \times 10 \times 0.6 = 240\text{ N}
Gravity pulls the object back down along the slope with force mgsinθmg \sin\theta.
2
Calculate the normal reaction force perpendicular to the plane
N=mgcosθ=40×10×0.8=320 NN = mg \cos\theta = 40 \times 10 \times 0.8 = 320\text{ N}
The normal force balances the perpendicular weight component.
3
Determine the magnitude of kinetic friction force
fk=μN=0.25×320=80 Nf_k = \mu N = 0.25 \times 320 = 80\text{ N}
Friction opposes motion up the slope and depends on the normal force.
4
Calculate the total pulling force needed for zero net acceleration
F=Fg+fk=240+80=320 NF = F_g + f_k = 240 + 80 = 320\text{ N}
At constant velocity, net force along the incline must equal zero, so F=mgsinθ+fkF = mg\sin\theta + f_k.
5
Calculate the power output of the conveyor
P=F×v=320 N×3 m s1=960 WP = F \times v = 320\text{ N} \times 3\text{ m s}^{-1} = 960\text{ W}
Power developed by a constant force moving an object at velocity vv is given by P=FvP = Fv.

Anahtar Kavram

Work done against gravity and friction, and rate of doing work (Power P=FvP = Fv)
Soru 174Soru

A wheel and axle system consists of a wheel with a radius of 25 cm25\text{ cm} attached to an axle with a radius of 5 cm5\text{ cm}. What is the velocity ratio of this machine?

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Cevap: 5

Cevap

The velocity ratio of the machine is 5.
The velocity ratio (VR) of a wheel and axle is the ratio of the radius of the wheel (RR) to the radius of the axle (rr). Calculating 25 cm5 cm\frac{25\text{ cm}}{5\text{ cm}} gives a velocity ratio of 55.

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1
Identify the formula for the velocity ratio of a wheel and axle system.
VR=Rr\text{VR} = \frac{R}{r}
Velocity ratio is defined as the distance moved by the effort (proportional to wheel radius) divided by the distance moved by the load (proportional to axle radius).
2
Substitute the given values into the formula.
VR=25 cm5 cm\text{VR} = \frac{25\text{ cm}}{5\text{ cm}}
The radius of the wheel R=25 cmR = 25\text{ cm} and the radius of the axle r=5 cmr = 5\text{ cm}.
3
Calculate the final ratio.
VR=5\text{VR} = 5
Dividing 25 by 5 yields 5. The ratio is dimensionless because the units of centimeters cancel out.

Anahtar Kavram

Velocity Ratio of a Wheel and Axle
Soru 175Soru

A uniform horizontal wooden rod XYXY of length 3.0 m3.0\text{ m} and weight 50 N50\text{ N} rests horizontally on two smooth supports located at XX (the left end) and at a point ZZ which is 0.6 m0.6\text{ m} from end YY. A block of weight 120 N120\text{ N} is placed on the rod at a distance of 0.9 m0.9\text{ m} from end XX. What is the magnitude of the upward reaction force, in newtons, at support ZZ?

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Cevap: 76.25

Cevap

The magnitude of the upward reaction force at support ZZ is 76.25 N76.25\text{ N}.
Taking moments about support XX, the total clockwise moment is the sum of the moment due to the load (120 N×0.9 m=108 Nm120\text{ N} \times 0.9\text{ m} = 108\text{ N}\cdot\text{m}) and the weight of the rod (50 N×1.5 m=75 Nm50\text{ N} \times 1.5\text{ m} = 75\text{ N}\cdot\text{m}), giving 183 Nm183\text{ N}\cdot\text{m}. Equating this to the counterclockwise moment of the reaction force at ZZ (RZ×2.4 mR_Z \times 2.4\text{ m}) yields RZ=1832.4=76.25 NR_Z = \frac{183}{2.4} = 76.25\text{ N}.

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1
Identify the perpendicular distance of each force and support from pivot point XX.
Center of gravity position xcg=1.5 mx_{cg} = 1.5\text{ m}, load position xL=0.9 mx_{L} = 0.9\text{ m}, and support ZZ position xZ=3.00.6=2.4 mx_{Z} = 3.0 - 0.6 = 2.4\text{ m}.
Taking moments about XX requires knowing the exact moment arm for each force from XX.
2
Set up the equation for rotational equilibrium about point XX.
Total clockwise moment = (120×0.9)+(50×1.5)=183 Nm(120 \times 0.9) + (50 \times 1.5) = 183\text{ N}\cdot\text{m}; Total counterclockwise moment = RZ×2.4R_Z \times 2.4.
Choosing pivot XX eliminates the unknown reaction force RXR_X because its distance from XX is zero.
3
Equate clockwise moments to counterclockwise moments and solve for RZR_Z.
RZ=1832.4=76.25 NR_Z = \frac{183}{2.4} = 76.25\text{ N}.
For a body in rotational equilibrium, the algebraic sum of moments about any point must equal zero.

Anahtar Kavram

Principle of Moments and Rotational Equilibrium
Soru 176Soru

A wheel and axle machine has a wheel of radius 25 cm25\text{ cm} and an axle of radius 5 cm5\text{ cm}. If an effort force of 100 N100\text{ N} is applied to lift a load of 400 N400\text{ N}, what is the efficiency of the machine?

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Cevap: 80%80\%

Cevap

The efficiency of the wheel and axle machine is 80%80\%.
First, calculate the velocity ratio as the ratio of wheel radius to axle radius: VR=255=5\text{VR} = \frac{25}{5} = 5. Next, calculate mechanical advantage as load over effort: MA=400100=4\text{MA} = \frac{400}{100} = 4. Finally, calculate efficiency by dividing mechanical advantage by velocity ratio: Efficiency=45×100%=80%\text{Efficiency} = \frac{4}{5} \times 100\% = 80\%.

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1
Calculate the Velocity Ratio (VR) of the wheel and axle system
VR=Radius of WheelRadius of Axle=25 cm5 cm=5\text{VR} = \frac{\text{Radius of Wheel}}{\text{Radius of Axle}} = \frac{25\text{ cm}}{5\text{ cm}} = 5
For a wheel and axle, the velocity ratio is the ratio of the radius of the wheel to the radius of the axle.
2
Calculate the Mechanical Advantage (MA) of the machine
MA=LoadEffort=400 N100 N=4\text{MA} = \frac{\text{Load}}{\text{Effort}} = \frac{400\text{ N}}{100\text{ N}} = 4
Mechanical advantage measures the force magnification of a machine, defined as the ratio of load raised to effort applied.
3
Calculate the Efficiency of the machine
Efficiency=MAVR×100%=45×100%=80%\text{Efficiency} = \frac{\text{MA}}{\text{VR}} \times 100\% = \frac{4}{5} \times 100\% = 80\%
Efficiency is defined as the ratio of Mechanical Advantage to Velocity Ratio expressed as a percentage.

Anahtar Kavram

Efficiency of Simple Machines
Soru 177Soru

A hydraulic press has a small piston with a diameter of 4 cm4\text{ cm} and a large piston with a diameter of 20 cm20\text{ cm}. If an effort force of 80 N80\text{ N} applied to the small piston raises a load of 1500 N1500\text{ N} placed on the large piston, what is the efficiency of the machine?

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Cevap: 75.0%75.0\%

Cevap

The efficiency of the hydraulic press is 75.0%75.0\%.
The mechanical advantage is MA=150080=18.75MA = \frac{1500}{80} = 18.75. The velocity ratio for pistons of diameters 20 cm20\text{ cm} and 4 cm4\text{ cm} is VR=(204)2=25VR = \left(\frac{20}{4}\right)^2 = 25. Efficiency is MAVR×100%=18.7525×100%=75.0%\frac{MA}{VR} \times 100\% = \frac{18.75}{25} \times 100\% = 75.0\%.

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1
Calculate Mechanical Advantage (MA)
MA=LoadEffort=1500 N80 N=18.75MA = \frac{\text{Load}}{\text{Effort}} = \frac{1500\text{ N}}{80\text{ N}} = 18.75
Mechanical advantage is defined as the ratio of load force to effort force.
2
Calculate Velocity Ratio (VR) for the hydraulic press
VR=A2A1=(d2d1)2=(20 cm4 cm)2=52=25VR = \frac{A_2}{A_1} = \left(\frac{d_2}{d_1}\right)^2 = \left(\frac{20\text{ cm}}{4\text{ cm}}\right)^2 = 5^2 = 25
The velocity ratio of a hydraulic press equals the ratio of the cross-sectional areas of the pistons, which simplifies to the square of the ratio of their diameters.
3
CalculateEfficiency(η)Calculate Efficiency (\eta)
\eta = \frac{MA}{VR} \times 100\% = \frac{18.75}{25} \times 100\% = 75.0\%
Efficiency is the ratio of mechanical advantage to velocity ratio expressed as a percentage.

Anahtar Kavram

Hydraulic Press Efficiency and Velocity Ratio
Soru 178Soru

A light, rigid horizontal bar ABAB of length 1.5 m1.5\text{ m} is smoothly pivoted at end AA. A vertical downward load of 40 N40\text{ N} is hung from end BB. The bar is kept in horizontal equilibrium by a light string attached at point CC, located 1.0 m1.0\text{ m} from AA. The string exerts a tension force TT pulling upwards at an angle of 3030^\circ relative to the horizontal bar. What is the magnitude of the tension TT in newtons?

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Cevap: 120

Cevap

The magnitude of the tension TT in the string is 120 N120\text{ N}.
For the bar to maintain rotational equilibrium, the clockwise moment about pivot AA must equal the counterclockwise moment about AA. The 40 N40\text{ N} load exerts a clockwise moment of 40 N×1.5 m=60 Nm40\text{ N} \times 1.5\text{ m} = 60\text{ N}\cdot\text{m}. The string tension TT exerts a counterclockwise moment given by its vertical component multiplied by the distance from the pivot: (Tsin30)×1.0 m=0.5T Nm(T \sin 30^\circ) \times 1.0\text{ m} = 0.5T \text{ N}\cdot\text{m}. Equating the two moments gives 0.5T=60 Nm0.5T = 60\text{ N}\cdot\text{m}, yielding T=120 NT = 120\text{ N}.

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1
Calculate the clockwise moment about the pivot at end AA
τclockwise=40 N×1.5 m=60 Nmτ_{\text{clockwise}} = 40\text{ N} \times 1.5\text{ m} = 60\text{ N}\cdot\text{m}
The weight at BB acts vertically downward at a perpendicular distance of 1.5 m1.5\text{ m} from pivot AA.
2
Determine the perpendicular component of tension TT relative to the bar
F=Tsin30=0.5TF_{\perp} = T \sin 30^\circ = 0.5T
Only the component of force perpendicular to the bar produces a moment about the pivot.
3
Set up the counterclockwise moment about pivot AA
τcounterclockwise=(0.5T)×1.0 m=0.5T Nmτ_{\text{counterclockwise}} = (0.5T) \times 1.0\text{ m} = 0.5T \text{ N}\cdot\text{m}
The string is attached at point CC, which is 1.0 m1.0\text{ m} away from pivot AA.
4
Apply the principle of moments for rotational equilibrium and solve for TT
0.5T=60    T=120 N0.5T = 60 \implies T = 120\text{ N}
For rotational equilibrium, total clockwise moments must equal total counterclockwise moments about any pivot.

Anahtar Kavram

Principle of moments and rotational equilibrium for forces acting at non-perpendicular angles.
Tahmini Süre:1m 30s
Soru 179Soru

A car of mass 1200 kg1200\text{ kg} ascends a straight road inclined at an angle θ\theta to the horizontal, where sinθ=0.1\sin\theta = 0.1, at a steady speed of 15 m s115\text{ m s}^{-1}. If the total frictional resistance to motion is 400 N400\text{ N}, what is the useful mechanical power output of the engine in kilowatts? (Take g=10 m s2g = 10\text{ m s}^{-2})

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Cevap: 24

Cevap

24 kW
To maintain a constant ascending speed, the engine must supply a force equal to the sum of the component of weight parallel to the incline (mgsinθ=1200 Nmg\sin\theta = 1200\text{ N}) and the frictional force (400 N400\text{ N}), resulting in a total force of 1600 N1600\text{ N}. Multiplying this total force by the constant speed of 15 m s115\text{ m s}^{-1} yields a power output of 24000 W24000\text{ W}, which corresponds to 24 kW24\text{ kW}.

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1
Calculate the gravitational force component acting down the slope
1200 N
The component of the car's weight parallel to the incline opposes upward motion: Fg=mgsinθ=1200 kg×10 m s2×0.1=1200 NF_g = m g \sin\theta = 1200 \text{ kg} \times 10 \text{ m s}^{-2} \times 0.1 = 1200 \text{ N}.
2
Determine the total tractive force required from the car engine
1600 N
Because the velocity is constant, the net force is zero; hence, the engine force must balance both the gravitational slope component and the frictional resistance: Fengine=Fg+Ffriction=1200 N+400 N=1600 NF_{\text{engine}} = F_g + F_{\text{friction}} = 1200 \text{ N} + 400 \text{ N} = 1600 \text{ N}.
3
Calculate the mechanical power delivered by the engine
24 kW
Power is the product of tractive force and constant speed: P=Fengine×v=1600 N×15 m s1=24000 W=24 kWP = F_{\text{engine}} \times v = 1600 \text{ N} \times 15 \text{ m s}^{-1} = 24000 \text{ W} = 24 \text{ kW}.

Anahtar Kavram

Power required to maintain motion against opposing forces on an inclined plane
Soru 180Soru

A porter carries a suitcase of mass 5 kg5\text{ kg} along a horizontal platform for a distance of 10 m10\text{ m} at a constant speed, and then lifts it vertically upward through a height of 2 m2\text{ m} onto a shelf. Taking g=10 m s2g = 10\text{ m s}^{-2}, what is the total work done by the porter on the suitcase?

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Cevap: 100 J100\text{ J}

Cevap

100 J100\text{ J}
During horizontal motion at constant speed, the upward force exerted by the porter is perpendicular to the horizontal displacement, so no work is performed horizontally (Whorizontal=Fscos90=0 JW_{\text{horizontal}} = F s \cos 90^\circ = 0\text{ J}). During vertical lifting, the force acts in the direction of displacement, yielding Wvertical=mgh=5 kg×10 m s2×2 m=100 JW_{\text{vertical}} = mgh = 5\text{ kg} \times 10\text{ m s}^{-2} \times 2\text{ m} = 100\text{ J}. The total work done is therefore 100 J100\text{ J}.

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1
Calculate the work done during horizontal motion
Whorizontal=0 JW_{\text{horizontal}} = 0\text{ J}
The supporting force acts vertically upward at an angle of 9090^\circ to the horizontal displacement, giving W=Fscos90=0 JW = F s \cos 90^\circ = 0\text{ J}.
2
Calculate the work done in lifting the suitcase vertically
Wvertical=mgh=5×10×2=100 JW_{\text{vertical}} = mgh = 5 \times 10 \times 2 = 100\text{ J}
Work done against gravity equals the increase in gravitational potential energy.
3
Sum the work done in both stages
Wtotal=0+100=100 JW_{\text{total}} = 0 + 100 = 100\text{ J}
Total work done is the scalar sum of work performed along each segment of motion.

Anahtar Kavram

Work done by a constant force depends on the direction of displacement (W=FscosθW = F s \cos \theta). Perpendicular forces do no work.
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