Mechanics

227 questions

Question 81Question

If two objects of unequal mass experience the same magnitude of net force for the same duration of time, the lighter object will undergo a greater change in linear momentum than the heavier object.

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Answer: False

Answer

The statement is False. Both objects undergo the exact same change in linear momentum because impulse depends only on the force applied and the time duration, not on the mass of the object.
The statement is false because the change in momentum (Δp\Delta p) is determined solely by the impulse applied (FΔtF \Delta t). Since the net force and time duration are identical for both objects, the change in momentum is the same for both, regardless of mass differences.

Step-by-Step Solution

1
State the relationship between force, time, and momentum change using Newton's Second Law.
Impulse J=FΔt=ΔpJ = F \Delta t = \Delta p, where FF is the net force, Δt\Delta t is the duration, and Δp\Delta p is the change in linear momentum.
The impulse-momentum theorem directly links the net force acting over time to the resulting change in momentum.
2
Evaluate the given problem constraints for both the lighter mass (m1m_1) and heavier mass (m2m_2).
F1=F2=FF_1 = F_2 = F and Δt1=Δt2=Δt\Delta t_1 = \Delta t_2 = \Delta t.
Both objects experience equal forces for equal durations.
3
Compare the resulting changes in linear momentum.
Δp1=FΔt\Delta p_1 = F \Delta t and Δp2=FΔt\Delta p_2 = F \Delta t, so Δp1=Δp2\Delta p_1 = \Delta p_2.
Because mass mm does not alter the product FΔtF \Delta t, both objects experience identical momentum changes.

Key Concept

Impulse-Momentum Theorem and Newton's Second Law of Motion
Question 82Question

A sledge of mass 8.0 kg8.0\text{ kg} sliding on ice with an initial velocity of 15 m s115\text{ m s}^{-1} enters a rough patch that exerts a constant retarding force of 24 N24\text{ N}. Calculate the time, in seconds, required for the sledge to come to a complete stop.

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Answer: 5

Answer

The time required for the sledge to come to a complete stop is 5.0 s5.0\text{ s}.
By Newton's second law in terms of momentum, the rate of change of momentum is equal to the applied net force (F=ΔpΔtF = \frac{\Delta p}{\Delta t}). Rearranging gives Δt=m(vu)F\Delta t = \frac{m(v - u)}{F}. Substituting m=8.0 kgm = 8.0\text{ kg}, u=15 m s1u = 15\text{ m s}^{-1}, v=0 m s1v = 0\text{ m s}^{-1}, and retarding force F=24 NF = -24\text{ N} yields Δt=8.0×(015)24=5.0 s\Delta t = \frac{8.0 \times (0 - 15)}{-24} = 5.0\text{ s}.

Step-by-Step Solution

1
Determine the change in linear momentum of the sledge.
The change in linear momentum is Δp=m(vu)=8.0 kg×(0 m s115 m s1)=120 kg m s1\Delta p = m(v - u) = 8.0\text{ kg} \times (0\text{ m s}^{-1} - 15\text{ m s}^{-1}) = -120\text{ kg m s}^{-1}.
Linear momentum is defined as the product of mass and velocity.
2
Apply the impulse-momentum theorem to determine the time duration.
Δt=ΔpF=120 kg m s124 N=5.0 s\Delta t = \frac{\Delta p}{F} = \frac{-120\text{ kg m s}^{-1}}{-24\text{ N}} = 5.0\text{ s}.
Impulse delivered by a net force over a time interval equals the change in linear momentum.

Key Concept

Newton's Second Law and Impulse-Momentum Theorem
Question 83Question

A spring with a force constant of 400 N m1400\text{ N m}^{-1} is compressed by 0.1 m0.1\text{ m} from its uncompressed length. When released, it launches a block of mass 0.16 kg0.16\text{ kg} along a smooth horizontal surface. What is the speed of the block immediately after leaving the spring?

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Answer: 5.0 m s15.0\text{ m s}^{-1}

Answer

The speed of the block immediately after leaving the spring is 5.0 m s15.0\text{ m s}^{-1}.
According to the principle of conservation of mechanical energy, the elastic potential energy stored in the compressed spring (Ep=12kx2E_p = \frac{1}{2} k x^2) is completely converted into kinetic energy (Ek=12mv2E_k = \frac{1}{2} m v^2) when the spring is released on a frictionless surface. Substituting k=400 N m1k = 400\text{ N m}^{-1}, x=0.1 mx = 0.1\text{ m}, and m=0.16 kgm = 0.16\text{ kg} yields 2.0 J=0.08v22.0\text{ J} = 0.08 v^2, which solves to v=5.0 m s1v = 5.0\text{ m s}^{-1}.

Step-by-Step Solution

1
Calculate the elastic potential energy stored in the compressed spring.
Ep=12kx2=12×400×(0.1)2=200×0.01=2.0 JE_p = \frac{1}{2} k x^2 = \frac{1}{2} \times 400 \times (0.1)^2 = 200 \times 0.01 = 2.0\text{ J}
Work done in compressing the spring is stored as elastic potential energy.
2
Apply conservation of mechanical energy.
Ek=Ep    12mv2=2.0 JE_k = E_p \implies \frac{1}{2} m v^2 = 2.0\text{ J}
Since the surface is smooth, all potential energy transforms into kinetic energy.
3
Solve for the velocity vv of the block.
12×0.16×v2=2.0    0.08v2=2.0    v2=25    v=5.0 m s1\frac{1}{2} \times 0.16 \times v^2 = 2.0 \implies 0.08 v^2 = 2.0 \implies v^2 = 25 \implies v = 5.0\text{ m s}^{-1}
Isolate vv by dividing by 0.080.08 and taking the square root.

Key Concept

Conservation of Mechanical Energy (Elastic Potential Energy to Kinetic Energy)
Question 84Question

A crate is pulled along a smooth horizontal floor by a constant force of 80 N80\text{ N} applied at an angle of 6060^\circ to the horizontal. If the crate moves through a displacement of 15 m15\text{ m} along the floor, what is the work done by the applied force?

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Answer: 600 J600\text{ J}

Answer

600 J600\text{ J}
The work done by a constant force applied at an angle θ\theta to the direction of motion is given by W=FscosθW = F s \cos\theta. Substituting F=80 NF = 80\text{ N}, s=15 ms = 15\text{ m}, and cos(60)=0.5\cos(60^\circ) = 0.5 gives W=80×15×0.5=600 JW = 80 \times 15 \times 0.5 = 600\text{ J}.

Step-by-Step Solution

1
Identify the given physical quantities
Force F=80 NF = 80\text{ N}, displacement s=15 ms = 15\text{ m}, angle θ=60\theta = 60^\circ
Extract parameters required for the work formula.
2
Apply the work formula for a force at an angle
W=FscosθW = F s \cos\theta
Only the component of force parallel to the displacement does work on the object.
3
Substitute the values and compute the result
W=80×15×cos(60)=1200×0.5=600 JW = 80 \times 15 \times \cos(60^\circ) = 1200 \times 0.5 = 600\text{ J}
Calculates the effective work done by the applied force.

Key Concept

Work Done by a Constant Force at an Angle
Estimated Time:1m 0s
Question 85Question

An electric motor with an efficiency of 80%80\% is used to pull a 100 kg100\text{ kg} object up a smooth incline inclined at 3030^\circ to the horizontal at a constant speed of 2 m s12\text{ m s}^{-1}. Taking acceleration due to gravity g=10 m s2g = 10\text{ m s}^{-2}, what is the electrical power input to the motor, in watts?

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Answer: 1250

Answer

1250 W
The force needed to move the mass up the smooth incline at constant speed is the parallel component of weight, F=mgsin(30)=500 NF = mg \sin(30^\circ) = 500\text{ N}. The useful power output is Pout=Fv=500×2=1000 WP_{\text{out}} = Fv = 500 \times 2 = 1000\text{ W}. Dividing by the efficiency of 0.800.80 yields the electrical power input Pin=1250 WP_{\text{in}} = 1250\text{ W}.

Step-by-Step Solution

1
Determine the force required along the inclined plane.
F=mgsin(30)=100 kg×10 m s2×0.5=500 NF = mg \sin(30^\circ) = 100\text{ kg} \times 10\text{ m s}^{-2} \times 0.5 = 500\text{ N}
At constant velocity, the applied force balances the component of weight parallel to the incline.
2
Calculate the useful power output delivered by the motor.
Pout=F×v=500 N×2 m s1=1000 WP_{\text{out}} = F \times v = 500\text{ N} \times 2\text{ m s}^{-1} = 1000\text{ W}
Mechanical power output is the product of pulling force and constant speed.
3
Calculate the total electrical power input required.
Pin=PoutEfficiency=1000 W0.80=1250 WP_{\text{in}} = \frac{P_{\text{out}}}{\text{Efficiency}} = \frac{1000\text{ W}}{0.80} = 1250\text{ W}
Efficiency is defined as the ratio of useful power output to total power input.

Key Concept

Mechanical power on inclined planes and system efficiency
Question 86Question

A water pump raises 600 kg600\text{ kg} of water through a vertical height of 20 m20\text{ m} in 50 s50\text{ s}. If the efficiency of the pump is 80%80\%, what is the electrical power input required to operate the pump? (Take g=10 m s2g = 10\text{ m s}^{-2})

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Answer: 3.0 kW3.0\text{ kW}

Answer

3.0 kW3.0\text{ kW}
The correct answer is 3.0 kW3.0\text{ kW}. Raising 600 kg600\text{ kg} of water by 20 m20\text{ m} requires 120,000 J120,000\text{ J} of gravitational potential energy. Doing this in 50 s50\text{ s} requires an output power of 2,400 W2,400\text{ W} (2.4 kW2.4\text{ kW}). Since the pump operates at 80%80\% efficiency, the input power must be 2.4 kW0.80=3.0 kW\frac{2.4\text{ kW}}{0.80} = 3.0\text{ kW}.

Step-by-Step Solution

1
Calculate the useful work output needed to elevate the water
Wout=mgh=600 kg×10 m s2×20 m=120,000 JW_{out} = mgh = 600\text{ kg} \times 10\text{ m s}^{-2} \times 20\text{ m} = 120,000\text{ J}
Work done against gravity equals the gravitational potential energy gained
2
Calculate the useful output power of the pump
Pout=Woutt=120,000 J50 s=2,400 W=2.4 kWP_{out} = \frac{W_{out}}{t} = \frac{120,000\text{ J}}{50\text{ s}} = 2,400\text{ W} = 2.4\text{ kW}
Power is defined as the rate at which work is performed
3
Calculate the required electrical power input using efficiency
Pin=PoutEfficiency=2.4 kW0.80=3.0 kWP_{in} = \frac{P_{out}}{\text{Efficiency}} = \frac{2.4\text{ kW}}{0.80} = 3.0\text{ kW}
Efficiency is the ratio of useful output power to total input power

Key Concept

Work done against gravity, power, and mechanical/electrical efficiency
Estimated Time:1m 30s
Question 87Question

A constant horizontal force acts on a body of mass 10 kg10\text{ kg}, accelerating it from rest to a speed of 12 m s112\text{ m s}^{-1} in a time of 4 s4\text{ s} along a smooth horizontal surface. What is the average power delivered by the force during this time interval?

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Answer: 180

Answer

The average power delivered by the force during the 4-second interval is 180 W180\text{ W}.
By the work-energy theorem, the total work done by the constant force equals the gain in kinetic energy: W=12mv2=12×10×144=720 JW = \frac{1}{2} m v^2 = \frac{1}{2} \times 10 \times 144 = 720\text{ J}. The average power is the rate at which work is performed over time: P=Wt=720 J4 s=180 WP = \frac{W}{t} = \frac{720\text{ J}}{4\text{ s}} = 180\text{ W}.

Step-by-Step Solution

1
Calculate the final kinetic energy acquired by the body.
Ek=12mv2=12(10 kg)(12 m s1)2=720 JE_k = \frac{1}{2} m v^2 = \frac{1}{2} (10\text{ kg})(12\text{ m s}^{-1})^2 = 720\text{ J}.
Since the body starts from rest on a smooth surface, all work done by the net force goes into increasing its kinetic energy.
2
Divide the total work done by the elapsed time to find the average power.
Pavg=Wt=720 J4 s=180 WP_{\text{avg}} = \frac{W}{t} = \frac{720\text{ J}}{4\text{ s}} = 180\text{ W}.
Average power is defined as the rate of doing work over a given time interval.

Key Concept

Work-Energy Theorem and Average Power
Question 88Question

A hydraulic press consists of a small effort piston of radius 2 cm2\text{ cm} and a large load piston of radius 8 cm8\text{ cm}. When an effort force of 50 N50\text{ N} is applied to the small piston, it successfully lifts a load of 600 N600\text{ N} placed on the large piston. What is the efficiency of this hydraulic press?

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Answer: 75%75\%

Answer

The efficiency of the hydraulic press is 75%75\%.
The correct answer is 75%75\%. The mechanical advantage is MA=60050=12MA = \frac{600}{50} = 12, and the velocity ratio is VR=(82)2=16VR = \left(\frac{8}{2}\right)^2 = 16. Taking the ratio MAVR×100%\frac{MA}{VR} \times 100\% yields 1216×100%=75%\frac{12}{16} \times 100\% = 75\%.

Step-by-Step Solution

1
Calculate the Mechanical Advantage (MA) of the hydraulic press.
MA=LoadEffort=600 N50 N=12MA = \frac{\text{Load}}{\text{Effort}} = \frac{600\text{ N}}{50\text{ N}} = 12
Mechanical advantage measures the force multiplication factor of a machine.
2
Calculate the Velocity Ratio (VR) of the hydraulic press using the piston radii.
VR=Area of load pistonArea of effort piston=πR2πr2=(8 cm2 cm)2=42=16VR = \frac{\text{Area of load piston}}{\text{Area of effort piston}} = \frac{\pi R^2}{\pi r^2} = \left(\frac{8\text{ cm}}{2\text{ cm}}\right)^2 = 4^2 = 16
For a hydraulic press, velocity ratio equals the ratio of the cross-sectional areas of the pistons, which simplifies to the square of the radii ratio.
3
Compute the efficiency of the machine.
η=MAVR×100%=1216×100%=75%\eta = \frac{MA}{VR} \times 100\% = \frac{12}{16} \times 100\% = 75\%
Efficiency is defined as the ratio of Mechanical Advantage to Velocity Ratio expressed as a percentage.

Key Concept

Mechanical Advantage, Velocity Ratio, and Efficiency of a Hydraulic Press
Estimated Time:1m 30s
Question 89Question

A block and tackle system consisting of 55 pulleys is used to raise a load of 200 N200\text{ N} through a vertical height of 4 m4\text{ m}. If the efficiency of the system is 80%80\%, what is the work done against friction, in joules, during the lifting process?

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Answer: 200

Answer

The work done against friction during the lifting process is 200 J200\text{ J}.
The useful work output is achieved by lifting the 200 N200\text{ N} load through a vertical height of 4 m4\text{ m}, yielding Wout=200×4=800 JW_{\text{out}} = 200 \times 4 = 800\text{ J}. Given an efficiency of 80%80\% (0.800.80), the total work input required from the effort force is Win=8000.80=1000 JW_{\text{in}} = \frac{800}{0.80} = 1000\text{ J}. The energy lost to overcome frictional resistance in the pulleys equals the total work input minus useful work output: 1000 J800 J=200 J1000\text{ J} - 800\text{ J} = 200\text{ J}.

Step-by-Step Solution

1
Calculate useful work output
Wout=800 JW_{\text{out}} = 800\text{ J}
Useful work output is the energy required to raise the load through the specified height (Wout=Load×heightW_{\text{out}} = \text{Load} \times \text{height}).
2
Determine total work input
Win=1000 JW_{\text{in}} = 1000\text{ J}
The total work input is calculated from the efficiency formula: Efficiency=WoutWin\text{Efficiency} = \frac{W_{\text{out}}}{W_{\text{in}}}.
3
Compute work done against friction
Wfriction=200 JW_{\text{friction}} = 200\text{ J}
The work lost overcoming friction is the difference between total work input and useful work output (WinWoutW_{\text{in}} - W_{\text{out}}).

Key Concept

Work and Efficiency in Pulley Systems
Estimated Time:1m 30s
Question 90Question

A machine with a velocity ratio of 66 is used to raise a load of 540 N540\text{ N} by applying an effort of 120 N120\text{ N}. What is the efficiency of the machine?

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Answer: 75%75\%

Answer

The efficiency of the machine is 75%75\%.
The correct option is 75%75\%. Mechanical Advantage is found by dividing the load (540 N540\text{ N}) by the effort (120 N120\text{ N}), giving 4.54.5. Dividing this mechanical advantage by the given velocity ratio (66) and expressing as a percentage yields 4.56×100%=75%\frac{4.5}{6} \times 100\% = 75\%.

Step-by-Step Solution

1
Calculate Mechanical Advantage (MA)
MA=LoadEffort=540 N120 N=4.5\text{MA} = \frac{\text{Load}}{\text{Effort}} = \frac{540\text{ N}}{120\text{ N}} = 4.5
Mechanical advantage measures the force magnification produced by the machine.
2
CalculateEfficiency(η)Calculate Efficiency (\eta)
η=(MAVR)×100%=(4.56)×100%=75%\eta = \left(\frac{\text{MA}}{\text{VR}}\right) \times 100\% = \left(\frac{4.5}{6}\right) \times 100\% = 75\%
Efficiency is the ratio of Mechanical Advantage to Velocity Ratio multiplied by 100%.

Key Concept

Efficiency of a Simple Machine
Estimated Time:1m 0s
Question 91Question

An inclined plane is set at an angle of 3030^\circ to the horizontal. An effort of 320 N320\text{ N} applied parallel to the plane is used to push a load of 480 N480\text{ N} up the incline at a constant speed. What is the efficiency of the inclined plane expressed as a percentage?

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Answer: 75%; 75; 75 percent

Answer

The efficiency of the inclined plane is 75%75\%.
For an inclined plane inclined at 3030^\circ to the horizontal, the velocity ratio (VR) is given by VR=1sin30=2\text{VR} = \frac{1}{\sin 30^\circ} = 2. The mechanical advantage (MA) is MA=LoadEffort=480 N320 N=1.5\text{MA} = \frac{\text{Load}}{\text{Effort}} = \frac{480\text{ N}}{320\text{ N}} = 1.5. Dividing MA by VR and multiplying by 100%100\% yields an efficiency of (1.52)×100%=75%\left(\frac{1.5}{2}\right) \times 100\% = 75\%.

Step-by-Step Solution

1
Determine the Velocity Ratio (VR) of the inclined plane from its angle of inclination
VR = \frac{1}{\sin 30^\circ} = \frac{1}{0.5} = 2
For an inclined plane with inclination angle \theta, the velocity ratio is equal to \frac{1}{\sin \theta}.
2
Calculate the Mechanical Advantage (MA)
MA = \frac{\text{Load}}{\text{Effort}} = \frac{480\text{ N}}{320\text{ N}} = 1.5
Mechanical advantage is defined as the ratio of load to effort force.
3
Calculate the efficiency of the machine
\text{Efficiency} = \frac{\text{MA}}{\text{VR}} \times 100\% = \frac{1.5}{2} \times 100\% = 75\%
Efficiency is the ratio of mechanical advantage to velocity ratio expressed as a percentage.

Key Concept

Efficiency of an Inclined Plane
Question 92Question

A light rigid bar PQPQ of length 5.0 m5.0\text{ m} is hinged at end PP and held horizontally. An upward force of 40 N40\text{ N} is applied at end QQ at an angle of 3030^\circ to the bar. To keep the bar in horizontal equilibrium, a vertical downward force FF is applied at a distance of 2.0 m2.0\text{ m} from PP. What is the magnitude of the force FF?

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Answer: 50 N50\text{ N}

Answer

The magnitude of the force FF required to maintain equilibrium is 50 N50\text{ N}.
The force of 40 N40\text{ N} applied at an angle of 3030^\circ to the bar has a perpendicular component of 40sin30=20 N40\sin 30^\circ = 20\text{ N}. The counterclockwise moment about pivot PP is 20 N×5.0 m=100 Nm20\text{ N} \times 5.0\text{ m} = 100\text{ N}\cdot\text{m}. For the bar to remain in equilibrium, the clockwise moment created by FF must equal 100 Nm100\text{ N}\cdot\text{m}, giving F×2.0 m=100 NmF \times 2.0\text{ m} = 100\text{ N}\cdot\text{m}, which yields F=50 NF = 50\text{ N}.

Step-by-Step Solution

1
Calculate the perpendicular component of the force applied at end QQ.
F=40 N×sin(30)=40×0.5=20 NF_{\perp} = 40\text{ N} \times \sin(30^\circ) = 40 \times 0.5 = 20\text{ N}
Only the force component perpendicular to the bar produces a moment about the pivot PP.
2
Calculate the counterclockwise moment produced by the force at QQ about pivot PP.
\text{Moment}_{Q} = 20\text{ N} \times 5.0\text{ m} = 100\text{ N}\cdot\text{m}
Moment is defined as perpendicular force multiplied by distance from the pivot.
3
Apply the Principle of Moments about pivot PP to find force FF.
F \times 2.0\text{ m} = 100\text{ N}\cdot\text{m} \implies F = \frac{100}{2.0} = 50\text{ N}
For rotational equilibrium, total clockwise moment about PP must equal total counterclockwise moment about PP.

Key Concept

Principle of Moments and Rotational Equilibrium with Forces at an Angle
Question 93Question

A uniform horizontal wooden beam ABAB of length 4.0 m4.0\text{ m} and mass 8.0 kg8.0\text{ kg} is supported on a pivot placed 1.0 m1.0\text{ m} from end AA. A mass of 5.0 kg5.0\text{ kg} is suspended from end BB. What is the magnitude of the downward vertical force FF in newtons that must be applied at end AA to keep the beam in horizontal equilibrium? (Take g=10 m/s2g = 10\text{ m/s}^2).

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Answer: 230

Answer

The magnitude of the downward force required at end A to maintain horizontal equilibrium is 230 N.
Taking moments about the pivot, the downward force F at end A produces an anticlockwise moment of F × 1.0 m. This balances the clockwise moments produced by the weight of the beam (80 N × 1.0 m) and the load at end B (50 N × 3.0 m). Equating anticlockwise and clockwise moments gives F × 1.0 = 80 + 150 = 230 N.

Step-by-Step Solution

1
Determine the weights and distance of each force from the pivot point
Weight of beam = 80 N acting at 1.0 m right of pivot; weight at B = 50 N acting at 3.0 m right of pivot; force F acts at 1.0 m left of pivot.
The center of gravity of a uniform 4.0 m beam is at its midpoint (2.0 m from end A).
2
Set up the moment equilibrium equation about the pivot
F × 1.0 = (80 × 1.0) + (50 × 3.0)
For static rotational equilibrium, total anticlockwise moments equal total clockwise moments.
3
Solve for the force magnitude F
F = 230 N
Summing clockwise moments yields 80 + 150 = 230 N m, which divided by 1.0 m gives F = 230 N.

Key Concept

Principle of Moments and Static Equilibrium
Estimated Time:1m 30s
Question 94Question

A uniform horizontal beam XYXY of length 3.0 m3.0\text{ m} and weight 80 N80\text{ N} is hinged at end XX to a vertical wall. It is held in horizontal equilibrium by a light cable attached to end YY that makes an angle of 3030^\circ with the beam. What is the tension in the cable?

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Answer: 80 N80\text{ N}

Answer

The tension in the cable is 80 N80\text{ N}.
Taking moments about the hinge at end XX, the clockwise moment due to the weight of the beam acting at its midpoint (1.5 m1.5\text{ m}) is 80 N×1.5 m=120 Nm80\text{ N} \times 1.5\text{ m} = 120\text{ N}\cdot\text{m}. The counterclockwise moment provided by the cable tension TT at end YY (3.0 m3.0\text{ m}) is Tsin(30)×3.0 m=1.5T NmT \sin(30^\circ) \times 3.0\text{ m} = 1.5 T\text{ N}\cdot\text{m}. Setting clockwise moments equal to counterclockwise moments gives 1.5T=1201.5 T = 120, yielding T=80 NT = 80\text{ N}.

Step-by-Step Solution

1
Identify the center of gravity and calculate the clockwise moment about the hinge at end XX.
Since the beam is uniform, its weight of 80 N80\text{ N} acts at its center of gravity, which is at a distance of 1.5 m1.5\text{ m} from XX. Clockwise moment = 80 N×1.5 m=120 Nm80\text{ N} \times 1.5\text{ m} = 120\text{ N}\cdot\text{m}.
For a uniform body, weight acts precisely at the midpoint.
2
Determine the counterclockwise moment exerted by the cable tension TT about point XX.
The perpendicular component of the tension is Tsin(30)T \sin(30^\circ). Counterclockwise moment = Tsin(30)×3.0 m=1.5T NmT \sin(30^\circ) \times 3.0\text{ m} = 1.5 T\text{ N}\cdot\text{m}.
Only the component of force perpendicular to the beam produces a moment about the pivot.
3
Apply the principle of moments for rotational equilibrium to solve for TT.
1.5T=120    T=1201.5=80 N1.5 T = 120 \implies T = \frac{120}{1.5} = 80\text{ N}.
For equilibrium, total counterclockwise moments about any pivot must equal total clockwise moments.

Key Concept

Principle of Moments and Rotational Equilibrium
Estimated Time:1m 30s
Question 95Question

A uniform horizontal plank ABAB of length 5.0 m5.0\text{ m} and mass 40 kg40\text{ kg} rests on two smooth supports, CC and DD, located 1.0 m1.0\text{ m} from end AA and 1.0 m1.0\text{ m} from end BB respectively. What is the maximum mass, in kilograms, of an object that can be placed at end AA without causing the plank to tilt?

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Answer: 60

Answer

The maximum mass that can be placed at end A without tilting the plank is 60 kg.
Just before tilting, the plank rotates around support C, causing the normal reaction at support D to drop to zero. Equating the anticlockwise moment of the added mass at end A about support C ((mg)×1.0 m(m \cdot g) \times 1.0\text{ m}) to the clockwise moment of the plank's weight about support C ((40g)×1.5 m(40 \cdot g) \times 1.5\text{ m}) yields m=60 kgm = 60\text{ kg}.

Step-by-Step Solution

1
Identify the tipping condition and pivot point
Support C acts as the pivot; the reaction at support D becomes zero (RD=0R_D = 0).
When extra weight is added at end A, the plank rotates about C and lifts off support D.
2
Calculate perpendicular distances from the pivot C
Distance to added mass mm = 1.0 m1.0\text{ m}; Distance to plank's center of mass = 2.5 m1.0 m=1.5 m2.5\text{ m} - 1.0\text{ m} = 1.5\text{ m}.
The weight of a uniform beam acts at its midpoint (2.5 m from either end).
3
Equate clockwise and counterclockwise moments about C
m×g×1.0 m=40 kg×g×1.5 mm \times g \times 1.0\text{ m} = 40\text{ kg} \times g \times 1.5\text{ m}, giving m=60 kgm = 60\text{ kg}.
For the plank to remain balanced just before tipping, total anticlockwise moment must equal total clockwise moment.

Key Concept

Rotational Equilibrium and Tilting of Rigid Bodies
Estimated Time:1m 30s
Question 96Question

A uniform rigid bar ABAB of length 2.0 m2.0\text{ m} and weight 120 N120\text{ N} is hinged smoothly at end AA to a vertical post. The bar is held in equilibrium at an angle of 6060^\circ above the horizontal by a force FF applied at end BB acting perpendicular to the bar. What is the magnitude of the force FF?

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Answer: 30 N30\text{ N}

Answer

The magnitude of the force required to keep the bar in equilibrium is 30 N30\text{ N}.
To maintain rotational equilibrium, the clockwise moment created by the weight of the bar about hinge AA must equal the counterclockwise moment created by force FF. The weight of 120 N120\text{ N} acts at the bar's midpoint (1.0 m1.0\text{ m} from AA), and its perpendicular distance to the vertical line of action is 1.0cos(60)=0.5 m1.0 \cos(60^\circ) = 0.5\text{ m}. Thus, the clockwise moment is 120×0.5=60 Nm120 \times 0.5 = 60\text{ N}\cdot\text{m}. Since force FF acts perpendicularly at the end of the 2.0 m2.0\text{ m} bar, its moment is F×2.0F \times 2.0. Setting 2.0F=602.0 F = 60 gives F=30 NF = 30\text{ N}.

Step-by-Step Solution

1
Identify the center of gravity and the position of applied forces.
For a uniform bar of length L=2.0 mL = 2.0\text{ m}, its weight W=120 NW = 120\text{ N} acts vertically downward at its center of gravity, which is at a distance of 1.0 m1.0\text{ m} from hinge AA.
The weight of a uniform body acts through its midpoint.
2
Determine the perpendicular distance for each force relative to the pivot at AA.
Perpendicular distance for weight: dW=1.0 m×cos(60)=0.5 md_W = 1.0\text{ m} \times \cos(60^\circ) = 0.5\text{ m}. Perpendicular distance for force FF: dF=2.0 md_F = 2.0\text{ m} (since FF is perpendicular to the bar).
The moment of a force is defined as the product of the force magnitude and the perpendicular distance from the pivot to the line of action of the force.
3
Apply the Principle of Moments about the pivot AA.
MA=0    F×2.0 m=120 N×0.5 m    2.0F=60    F=30 N\sum M_A = 0 \implies F \times 2.0\text{ m} = 120\text{ N} \times 0.5\text{ m} \implies 2.0 F = 60 \implies F = 30\text{ N}.
For rotational equilibrium, the total counterclockwise moment about any pivot must equal the total clockwise moment.

Key Concept

Principle of Moments and Rotational Equilibrium
Question 97Question

A simple pendulum of length LL with a bob of mass mm has a period of oscillation of 2.0 s2.0\text{ s}. If the mass of the bob is increased to 4m4m and the length of the pendulum string is increased to 4L4L, what is the new period of oscillation?

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Answer: 4.0 s4.0\text{ s}

Answer

The new period of oscillation is 4.0 s4.0\text{ s}.
The period of a simple pendulum undergoing simple harmonic motion is given by T=2πLgT = 2\pi \sqrt{\frac{L}{g}}. The mass of the bob does not enter the period formula, meaning changes to bob mass have zero effect on the period. When the length of the pendulum is quadrupled (L=4LL' = 4L), the new period becomes T=2π4Lg=2×(2πLg)=2TT' = 2\pi \sqrt{\frac{4L}{g}} = 2 \times \left(2\pi \sqrt{\frac{L}{g}}\right) = 2T. Since the original period was 2.0 s2.0\text{ s}, the new period is 2×2.0 s=4.0 s2 \times 2.0\text{ s} = 4.0\text{ s}.

Step-by-Step Solution

1
Identify the formula for the period of a simple pendulum.
The period is given by T=2πLgT = 2\pi \sqrt{\frac{L}{g}}.
The period of simple harmonic motion for a simple pendulum depends only on the length of the string LL and the acceleration due to gravity gg, and is independent of the mass of the bob mm.
2
Substitute the scaled values into the formula to find the new period TT'.
T=2π4Lg=2×(2πLg)=2TT' = 2\pi \sqrt{\frac{4L}{g}} = 2 \times \left(2\pi \sqrt{\frac{L}{g}}\right) = 2T.
Taking the square root of 4L4L factors out a multiplier of 4=2\sqrt{4} = 2, while the change in mass from mm to 4m4m has no effect on the period.
3
Calculate the numerical value of the new period.
T=2×2.0 s=4.0 sT' = 2 \times 2.0\text{ s} = 4.0\text{ s}.
Multiplying the initial period of 2.0 s2.0\text{ s} by 22 yields 4.0 s4.0\text{ s}.

Key Concept

Mass Independence and Length Relationship of a Simple Pendulum
Question 98Question

A uniform cylindrical rod of length 20 cm20\text{ cm} floats vertically in liquid XX of density 800 kg/m3800\text{ kg/m}^3 with 15 cm15\text{ cm} of its length submerged. When transferred to liquid YY, it floats vertically with 12 cm12\text{ cm} of its length submerged. What is the density of liquid YY?

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Answer: 1000 kg/m31000\text{ kg/m}^3

Answer

The density of liquid YY is 1000 kg/m31000\text{ kg/m}^3.
According to the Law of Flotation, a floating body displaces its own weight of liquid. Therefore, hXρX=hYρYh_X \rho_X = h_Y \rho_Y. Substituting 15 cm×800 kg/m3=12 cm×ρY15\text{ cm} \times 800\text{ kg/m}^3 = 12\text{ cm} \times \rho_Y yields ρY=1000 kg/m3\rho_Y = 1000\text{ kg/m}^3.

Step-by-Step Solution

1
Apply the Law of Flotation for a floating body of uniform cross-sectional area AA.
Weight of rod W=Upthrust=AhsubmergedρliquidgW = \text{Upthrust} = A \cdot h_{\text{submerged}} \cdot \rho_{\text{liquid}} \cdot g.
A floating body displaces a weight of fluid equal to its own total weight.
2
Equate the upthrust in liquid XX to the upthrust in liquid YY.
AhXρXg=AhYρYg    hXρX=hYρYA \cdot h_X \cdot \rho_X \cdot g = A \cdot h_Y \cdot \rho_Y \cdot g \implies h_X \cdot \rho_X = h_Y \cdot \rho_Y.
Since the rod is identical and floating freely in both liquids, its weight WW remains unchanged.
3
Substitute the known values (hX=15 cmh_X = 15\text{ cm}, ρX=800 kg/m3\rho_X = 800\text{ kg/m}^3, hY=12 cmh_Y = 12\text{ cm}) and solve for ρY\rho_Y.
ρY=hXρXhY=15×80012=1000 kg/m3\rho_Y = \frac{h_X \cdot \rho_X}{h_Y} = \frac{15 \times 800}{12} = 1000\text{ kg/m}^3.
Rearranging the linear equation yields the density of liquid YY.

Key Concept

Law of Flotation and Hydrometer Principle
Estimated Time:1m 15s
Question 99Question

In Newton's law of universal gravitation, the gravitational force FF between two point masses m1m_1 and m2m_2 separated by a distance rr is expressed as F=Gm1m2r2F = G \frac{m_1 m_2}{r^2}, where GG is the universal gravitational constant. What is the dimensional formula of GG in terms of mass (M\text{M}), length (L\text{L}), and time (T\text{T})?

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Answer: M1L3T2\text{M}^{-1}\text{L}^3\text{T}^{-2}

Answer

M1L3T2\text{M}^{-1}\text{L}^3\text{T}^{-2}
The dimensional formula of the universal gravitational constant GG is derived by expressing G=Fr2m1m2G = \frac{F r^2}{m_1 m_2}. Substituting the basic dimensions of force (MLT2\text{M}\text{L}\text{T}^{-2}), radius squared (L2\text{L}^2), and mass squared (M2\text{M}^2) gives (MLT2)(L2)M2=M1L3T2\frac{(\text{M}\text{L}\text{T}^{-2})(\text{L}^2)}{\text{M}^2} = \text{M}^{-1}\text{L}^3\text{T}^{-2}.

Step-by-Step Solution

1
Make GG the subject of the formula
G=Fr2m1m2G = \frac{F \cdot r^2}{m_1 \cdot m_2}
To analyze the dimensions of GG, isolate it on one side of the equation.
2
Substitute the fundamental dimensions for force, distance, and mass
[F] = \text{M}\text{L}\text{T}^{-2}, [r^2] = \text{L}^2, [m_1 m_2] = \text{M}^2
Force is mass times acceleration, giving dimensions MLT2\text{M}\text{L}\text{T}^{-2}, while distance squared gives L2\text{L}^2 and the product of two masses gives M2\text{M}^2.
3
Simplify the dimensional expression
[G] = \frac{(\text{M}\text{L}\text{T}^{-2}) \cdot \text{L}^2}{\text{M}^2} = \text{M}^{1-2} \text{L}^{1+2} \text{T}^{-2} = \text{M}^{-1}\text{L}^3\text{T}^{-2}
Apply laws of indices for fundamental dimensions M\text{M}, L\text{L}, and T\text{T}.

Key Concept

Dimensional Analysis of Physical Constants
Estimated Time:1m 15s
Question 100Question

A ball is thrown vertically upwards with an initial velocity of 30 m/s30\text{ m/s} from the edge of a cliff that is 35 m35\text{ m} above ground level. Taking the acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the total time elapsed before the ball hits the ground?

Show answer & explanation

Answer: 7.0 s7.0\text{ s}

Answer

The total time elapsed before the ball hits the ground is 7.0 s7.0\text{ s}.
Using the displacement equation s=ut12gt2s = ut - \frac{1}{2}gt^2 with downward taken as negative, the net displacement when the ball reaches the ground is 35 m-35\text{ m}. Setting up the equation: 35=30t5t2-35 = 30t - 5t^2, which simplifies to t26t7=0t^2 - 6t - 7 = 0. Factoring gives (t7)(t+1)=0(t - 7)(t + 1) = 0, yielding t=7.0 st = 7.0\text{ s}.

Step-by-Step Solution

1
Calculate the time taken (t1t_1) to reach maximum height
t1=ug=3010=3.0 st_1 = \frac{u}{g} = \frac{30}{10} = 3.0\text{ s}
At maximum height, the final vertical velocity is 0 m/s0\text{ m/s}.
2
Calculate the maximum height (hmaxh_{max}) reached above the cliff
hmax=u22g=3022(10)=45 mh_{max} = \frac{u^2}{2g} = \frac{30^2}{2(10)} = 45\text{ m}
Using the kinematic equation v2=u22ghv^2 = u^2 - 2gh.
3
Determine total height above ground and time (t2t_2) to fall to the ground
Total height H=35 m+45 m=80 mH = 35\text{ m} + 45\text{ m} = 80\text{ m}. t2=2Hg=2(80)10=4.0 st_2 = \sqrt{\frac{2H}{g}} = \sqrt{\frac{2(80)}{10}} = 4.0\text{ s}
The ball falls from rest from a peak height of 80 m80\text{ m}.
4
Calculate the total time of flight
ttotal=t1+t2=3.0 s+4.0 s=7.0 st_{total} = t_1 + t_2 = 3.0\text{ s} + 4.0\text{ s} = 7.0\text{ s}
The complete journey consists of ascending to the peak and descending to the ground.

Key Concept

Kinematics of Vertical Motion Under Gravity
Estimated Time:1m 30s
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