Work, Energy and Power

24 questions

Question 1Question

A mountain climber of mass 60 kg60\text{ kg} climbs a vertical height of 15 m15\text{ m} in a time of 30 s30\text{ s}. Taking the acceleration due to gravity g=10 m s2g = 10\text{ m s}^{-2}, calculate the average power expended by the climber in Watts.

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Answer: 300

Answer

The average power expended by the climber is 300 W300\text{ W}.
The work done in lifting a mass mm through vertical height hh is given by W=mgh=60×10×15=9000 JW = mgh = 60 \times 10 \times 15 = 9000\text{ J}. The average power is the rate of doing work, P=Wt=9000 J30 s=300 WP = \frac{W}{t} = \frac{9000\text{ J}}{30\text{ s}} = 300\text{ W}.

Step-by-Step Solution

1
Identify the given values and formula for work done against gravity.
Mass m=60 kgm = 60\text{ kg}, vertical displacement h=15 mh = 15\text{ m}, acceleration due to gravity g=10 m s2g = 10\text{ m s}^{-2}, and time t=30 st = 30\text{ s}. Work done formula: W=mghW = mgh.
The climber works against gravity to increase their potential energy by an amount equal to mghmgh.
2
Calculate the total work done.
W=60 kg×10 m s2×15 m=9000 JW = 60\text{ kg} \times 10\text{ m s}^{-2} \times 15\text{ m} = 9000\text{ J}.
Multiplying force (mgmg) by vertical distance (hh) yields work done in Joules.
3
Calculate the average power.
P=Wt=9000 J30 s=300 WP = \frac{W}{t} = \frac{9000\text{ J}}{30\text{ s}} = 300\text{ W}.
Power is defined as work done divided by the time interval (P=WtP = \frac{W}{t}).

Key Concept

Power as the rate of doing work against gravity
Estimated Time:45s
Question 2Question

A bullet of mass 20 g20\text{ g} is moving horizontally at a speed of 400 m s1400\text{ m s}^{-1}. It strikes a stationary block of wood and emerges from the opposite side with a speed of 100 m s1100\text{ m s}^{-1}. What is the magnitude of the work done by the bullet against the resistance of the block, in Joules?

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Answer: 1500

Answer

The magnitude of the work done by the bullet in penetrating the block is 1500 J1500\text{ J}.
According to the Work-Energy Theorem, the net work done on an object equals the change in its kinetic energy. The reduction in kinetic energy as the bullet slows from 400 m s1400\text{ m s}^{-1} to 100 m s1100\text{ m s}^{-1} equals the work done against the resistive force of the wooden block.

Step-by-Step Solution

1
Convert the mass of the bullet into standard SI units (kilograms)
m=201000=0.02 kgm = \frac{20}{1000} = 0.02\text{ kg}
The standard SI unit for mass in energy equations is the kilogram.
2
Determine the initial kinetic energy of the bullet before entering the block
Eki=12×0.02 kg×(400 m s1)2=1600 JE_{ki} = \frac{1}{2} \times 0.02\text{ kg} \times (400\text{ m s}^{-1})^2 = 1600\text{ J}
Kinetic energy is defined as Ek=12mv2E_k = \frac{1}{2} m v^2.
3
Determine the final kinetic energy of the bullet as it emerges from the block
Ekf=12×0.02 kg×(100 m s1)2=100 JE_{kf} = \frac{1}{2} \times 0.02\text{ kg} \times (100\text{ m s}^{-1})^2 = 100\text{ J}
The bullet loses speed upon passing through the block, reducing its kinetic energy.
4
Apply the Work-Energy Theorem to find the work done against resistive forces
W=ΔEk=1600 J100 J=1500 JW = \Delta E_k = 1600\text{ J} - 100\text{ J} = 1500\text{ J}
The net work done on the bullet equals its change in kinetic energy.

Key Concept

Work-Energy Theorem
Question 3Question

A water pump driven by an engine with an efficiency of 80%80\% raises water from an underground tank of depth 20 m20\text{ m} and discharges it through a nozzle of cross-sectional area 10 cm210\text{ cm}^2 at a steady speed of 10 m/s10\text{ m/s}. Taking the density of water as 1000 kg/m31000\text{ kg/m}^3 and acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the minimum input power rating (in W\text{W}) required for the engine?

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Answer: 3125

Answer

The minimum input power rating required for the engine is 3125 W3125\text{ W}.
The engine must supply power to lift 10 kg10\text{ kg} of water per second through a vertical height of 20 m20\text{ m} while accelerating it to 10 m/s10\text{ m/s}. The useful power output is 2000 W2000\text{ W} (potential) +500 W+ 500\text{ W} (kinetic) =2500 W= 2500\text{ W}. Accounting for an engine efficiency of 80%80\%, the total input power is 25000.80=3125 W\frac{2500}{0.80} = 3125\text{ W}.

Step-by-Step Solution

1
Determine the mass of water discharged per unit time (mass flow rate).
dmdt=ρ×A×v=1000 kg/m3×(10×104 m2)×10 m/s=10 kg/s\frac{dm}{dt} = \rho \times A \times v = 1000\text{ kg/m}^3 \times (10 \times 10^{-4}\text{ m}^2) \times 10\text{ m/s} = 10\text{ kg/s}
Water is moving through a cross-sectional area at a constant velocity.
2
Calculate the useful output power required to lift the water and impart kinetic energy.
Pout=dmdtgh+12dmdtv2=(10×10×20)+(12×10×102)=2000 W+500 W=2500 WP_{\text{out}} = \frac{dm}{dt} g h + \frac{1}{2} \frac{dm}{dt} v^2 = (10 \times 10 \times 20) + \left(\frac{1}{2} \times 10 \times 10^2\right) = 2000\text{ W} + 500\text{ W} = 2500\text{ W}
The engine must perform work against gravity to raise the water depth and provide kinetic energy for exit velocity.
3
Calculate the total input power using engine efficiency.
Pin=PoutEfficiency=2500 W0.80=3125 WP_{\text{in}} = \frac{P_{\text{out}}}{\text{Efficiency}} = \frac{2500\text{ W}}{0.80} = 3125\text{ W}
Efficiency is the ratio of useful power output to total power input.

Key Concept

Work-Energy Theorem applied to fluid flow and Power-Efficiency relations
Question 4Question

A body of mass 4 kg4\text{ kg} moves with a constant velocity of 5 m s15\text{ m s}^{-1}. Calculate the kinetic energy of the body in Joules.

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Answer: 50

Answer

The kinetic energy of the body is 50 J50\text{ J}.
The kinetic energy of an object in linear motion is calculated using Ek=12mv2E_k = \frac{1}{2} m v^2. Substituting m=4 kgm = 4\text{ kg} and v=5 m s1v = 5\text{ m s}^{-1} gives Ek=12×4×52=50 JE_k = \frac{1}{2} \times 4 \times 5^2 = 50\text{ J}.

Step-by-Step Solution

1
Identify the given physical quantities
Mass m=4 kgm = 4\text{ kg} and velocity v=5 m s1v = 5\text{ m s}^{-1}
Extract values provided in the problem statement.
2
Apply the formula for kinetic energy
Ek=12mv2E_k = \frac{1}{2} m v^2
Kinetic energy is defined as half the product of mass and the square of velocity.
3
Substitute values and solve
Ek=12×4×(5)2=50 JE_k = \frac{1}{2} \times 4 \times (5)^2 = 50\text{ J}
Perform arithmetic evaluation to get the final energy in Joules.

Key Concept

Kinetic Energy
Question 5Question

A block is pulled along a smooth horizontal table by a horizontal force of 30 N30\text{ N} through a displacement of 4 m4\text{ m}. At the same time, a vertical upward force of 40 N40\text{ N} acts on the block as it moves. What is the total work done on the block?

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Answer: 120 J120\text{ J}

Answer

The total work done on the block is 120 J120\text{ J}.
Work done is given by W=FdcosθW = F d \cos\theta. The horizontal force acts along the line of motion (θ=0\theta = 0^\circ), performing 30 N×4 m=120 J30\text{ N} \times 4\text{ m} = 120\text{ J} of work. The vertical force acts at an angle of 9090^\circ to the horizontal displacement, performing zero work because cos(90)=0\cos(90^\circ) = 0. Thus, the total work done is 120 J120\text{ J}.

Step-by-Step Solution

1
Identify the formula for work done by a constant force
W=Fdcos(θ)W = F \cdot d \cdot \cos(\theta)
Work is defined as the scalar product of force and displacement vectors.
2
Calculate work done by the horizontal force
Whorizontal=30 N×4 m×cos(0)=120 JW_{\text{horizontal}} = 30\text{ N} \times 4\text{ m} \times \cos(0^\circ) = 120\text{ J}
The horizontal force is in the exact direction of motion (θ=0\theta = 0^\circ).
3
Calculate work done by the vertical force
Wvertical=40 N×4 m×cos(90)=0 JW_{\text{vertical}} = 40\text{ N} \times 4\text{ m} \times \cos(90^\circ) = 0\text{ J}
The vertical force is perpendicular to the horizontal displacement (θ=90\theta = 90^\circ), so cos(90)=0\cos(90^\circ) = 0.
4
Sum the work done by all forces
Wtotal=120 J+0 J=120 JW_{\text{total}} = 120\text{ J} + 0\text{ J} = 120\text{ J}
Work is a scalar quantity, so total work is the algebraic sum of individual work values.

Key Concept

Work done by perpendicular forces is zero
Estimated Time:45s
Question 6Question

A variable force FF acts on a body moving along a straight horizontal path. The force increases linearly from 0 N0\text{ N} at position x=0 mx = 0\text{ m} to 20 N20\text{ N} at x=4 mx = 4\text{ m}, remains constant at 20 N20\text{ N} from x=4 mx = 4\text{ m} to x=7 mx = 7\text{ m}, and then decreases linearly back to 0 N0\text{ N} at x=10 mx = 10\text{ m}. What is the total work done by the force in Joules over the 10 m10\text{ m} displacement?

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Answer: 130

Answer

130 J
The work done by a variable force is equal to the total area under the force-displacement (FF-xx) graph. The region under the graph forms a trapezoid bounded by parallel sides of length 10 m10\text{ m} (total displacement) and 3 m3\text{ m} (constant force interval), with a height of 20 N20\text{ N}. Calculating the area yields W=12(10+3)×20=130 JW = \frac{1}{2}(10 + 3) \times 20 = 130\text{ J}.

Step-by-Step Solution

1
Relate work done to the force-displacement graph
Work done WW equals the total area under the FF-xx graph between x=0 mx = 0\text{ m} and x=10 mx = 10\text{ m}.
By definition, W=FdxW = \int F \, dx, which corresponds to the geometric area under the force-displacement curve.
2
Calculate the geometric area under each section of the graph
First section (00 to 4 m4\text{ m}): Triangle area = 12×4×20=40 J\frac{1}{2} \times 4 \times 20 = 40\text{ J}. Second section (44 to 7 m7\text{ m}): Rectangle area = (74)×20=60 J(7 - 4) \times 20 = 60\text{ J}. Third section (77 to 10 m10\text{ m}): Triangle area = 12×(107)×20=30 J\frac{1}{2} \times (10 - 7) \times 20 = 30\text{ J}.
Breaking down a complex piecewise curve into simple geometric shapes allows straightforward area evaluation without calculus.
3
Sum the areas of all sections
Total Work W=40 J+60 J+30 J=130 JW = 40\text{ J} + 60\text{ J} + 30\text{ J} = 130\text{ J}.
The total work done is the scalar sum of the work done across each contiguous segment of displacement.

Key Concept

Work Done by a Variable Force (Area under Force-Displacement Graph)
Question 7Question

A box of mass 2 kg2\text{ kg} slides down a rough inclined plane from a height of 5 m5\text{ m}. If it reaches the bottom of the incline with a speed of 6 m s16\text{ m s}^{-1}, what is the work done against friction during the descent? (Take g=10 m s2g = 10\text{ m s}^{-2})

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Answer: 64 J64\text{ J}

Answer

64 J64\text{ J}
According to the principle of conservation of energy, the work done against friction equals the loss in total mechanical energy. The initial potential energy is mgh=2×10×5=100 Jmgh = 2 \times 10 \times 5 = 100\text{ J}, and the final kinetic energy is 12mv2=12×2×62=36 J\frac{1}{2}mv^2 = \frac{1}{2} \times 2 \times 6^2 = 36\text{ J}. Subtracting final kinetic energy from initial potential energy yields 100 J36 J=64 J100\text{ J} - 36\text{ J} = 64\text{ J}.

Step-by-Step Solution

1
Calculate the initial potential energy (EpE_p) at height h=5 mh = 5\text{ m}.
Ep=mgh=2 kg×10 m s2×5 m=100 JE_p = mgh = 2\text{ kg} \times 10\text{ m s}^{-2} \times 5\text{ m} = 100\text{ J}
At the top of the incline, all mechanical energy is stored as gravitational potential energy.
2
Calculate the final kinetic energy (EkE_k) at the bottom where v=6 m s1v = 6\text{ m s}^{-1}.
Ek=12mv2=12×2 kg×(6 m s1)2=36 JE_k = \frac{1}{2}mv^2 = \frac{1}{2} \times 2\text{ kg} \times (6\text{ m s}^{-1})^2 = 36\text{ J}
At the bottom of the incline, the remaining mechanical energy is kinetic energy.
3
Apply the work-energy theorem to find the work done against friction (WfW_f).
Wf=EpEk=100 J36 J=64 JW_f = E_p - E_k = 100\text{ J} - 36\text{ J} = 64\text{ J}
The non-conservative friction force reduces the total mechanical energy by doing work against motion.

Key Concept

Work-Energy Theorem and Conservation of Energy with Friction
Question 8Question

A body of mass 2 kg2\text{ kg} is projected vertically upward from ground level with an initial speed of 30 m s130\text{ m s}^{-1}. During its entire flight, it experiences a constant resistive force due to air resistance of 5 N5\text{ N}. Taking g=10 m s2g = 10\text{ m s}^{-2}, calculate the kinetic energy of the body in Joules when it returns to the ground level.

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Answer: 540

Answer

The kinetic energy of the body when it returns to ground level is 540 J540\text{ J}.
At launch, the body possesses an initial kinetic energy of Ei=12(2)(30)2=900 JE_i = \frac{1}{2}(2)(30)^2 = 900\text{ J}. During ascent, both gravity (20 N20\text{ N}) and air resistance (5 N5\text{ N}) retard the motion, giving a net downward force of 25 N25\text{ N} and a deceleration of 12.5 m s212.5\text{ m s}^{-2}. The maximum height reached is h=3022(12.5)=36 mh = \frac{30^2}{2(12.5)} = 36\text{ m}. Since the body travels up and down, total distance covered is 72 m72\text{ m}. Non-conservative work done against air resistance is W=5 N×72 m=360 JW = 5\text{ N} \times 72\text{ m} = 360\text{ J}. Therefore, the remaining kinetic energy upon returning to the ground is 900 J360 J=540 J900\text{ J} - 360\text{ J} = 540\text{ J}.

Step-by-Step Solution

1
Calculate initial kinetic energy of launch
Ei=900 JE_i = 900\text{ J}
Kinetic energy is given by 12mu2=12(2 kg)(30 m s1)2=900 J\frac{1}{2}m u^2 = \frac{1}{2}(2\text{ kg})(30\text{ m s}^{-1})^2 = 900\text{ J}.
2
Determine maximum height reached during ascent
h=36 mh = 36\text{ m}
Net upward retarding force F=mg+Fair=20+5=25 NF = mg + F_{\text{air}} = 20 + 5 = 25\text{ N}, yielding a deceleration a=12.5 m s2a = 12.5\text{ m s}^{-2}. Using 0=u22ah0 = u^2 - 2ah, h=90025=36 mh = \frac{900}{25} = 36\text{ m}.
3
Calculate energy lost to air resistance over total trajectory
Wair=360 JW_{\text{air}} = 360\text{ J}
Air resistance acts continuously over both ascent and descent (total distance 2h=72 m2h = 72\text{ m}). Work dissipated =Fair×2h=5×72=360 J= F_{\text{air}} \times 2h = 5 \times 72 = 360\text{ J}.
4
Subtract non-conservative work loss from initial mechanical energy
Ef=540 JE_f = 540\text{ J}
By mechanical energy balance, final kinetic energy Ef=EiWair=900360=540 JE_f = E_i - W_{\text{air}} = 900 - 360 = 540\text{ J}.

Key Concept

Work-Energy Theorem and Mechanical Energy Dissipation by Non-Conservative Forces
Question 9Question

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 10Question

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 11Question

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 12Question

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 13Question

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 14Question

An electric crane lifts a load of 250 kg250\text{ kg} vertically upwards through a height of 12 m12\text{ m} in 10 s10\text{ s} at a constant speed. Taking the acceleration due to gravity g=10 m s2g = 10\text{ m s}^{-2}, what is the useful output power of the crane in watts?

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Answer: 3000

Answer

The useful output power of the crane is 3000 W3000\text{ W}.
The work done in lifting the load vertically is equal to the gravitational potential energy gained, W=mgh=250×10×12=30,000 JW = mgh = 250 \times 10 \times 12 = 30,000\text{ J}. Power is the rate of doing work, so P=Wt=30,00010=3000 WP = \frac{W}{t} = \frac{30,000}{10} = 3000\text{ W}.

Step-by-Step Solution

1
Identify the given values
Mass m=250 kgm = 250\text{ kg}, height h=12 mh = 12\text{ m}, time t=10 st = 10\text{ s}, acceleration due to gravity g=10 m s2g = 10\text{ m s}^{-2}.
Extract values needed for work and power calculations.
2
Calculate the work done in lifting the load
W=mgh=250 kg×10 m s2×12 m=30,000 JW = mgh = 250 \text{ kg} \times 10 \text{ m s}^{-2} \times 12 \text{ m} = 30,000\text{ J}.
The work done against gravity equals the gain in gravitational potential energy.
3
Calculate the power output
P=Wt=30,000 J10 s=3000 WP = \frac{W}{t} = \frac{30,000\text{ J}}{10\text{ s}} = 3000\text{ W}.
Power is defined as the rate at which work is done (P=WtP = \frac{W}{t}).

Key Concept

Power as the rate of doing work against gravity
Question 15Question

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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Answer: 200 J200\text{ J}

Answer

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}.

Step-by-Step Solution

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

Key Concept

Work Done by a Constant Force
Question 16Question

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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Answer: 4 J4\text{ J}

Answer

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}.

Step-by-Step Solution

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.

Key Concept

Kinetic Energy
Estimated Time:45s
Question 17Question

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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Answer: 960

Answer

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}.

Step-by-Step Solution

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.

Key Concept

Work done against gravity and friction, and rate of doing work (Power P=FvP = Fv)
Question 18Question

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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Answer: 24

Answer

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}.

Step-by-Step Solution

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}.

Key Concept

Power required to maintain motion against opposing forces on an inclined plane
Question 19Question

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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Answer: 100 J100\text{ J}

Answer

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}.

Step-by-Step Solution

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.

Key Concept

Work done by a constant force depends on the direction of displacement (W=FscosθW = F s \cos \theta). Perpendicular forces do no work.
Question 20Question

An object of mass 4 kg4\text{ kg} is released from rest at a height of 5 m5\text{ m} above the ground. Neglecting air resistance and taking g=10 m s2g = 10\text{ m s}^{-2}, what is its kinetic energy just before striking the ground?

Show answer & explanation

Answer: 200 J200\text{ J}

Answer

The kinetic energy of the object just before striking the ground is 200 J200\text{ J}.
The total mechanical energy is conserved during free fall. The initial gravitational potential energy Ep=mgh=4×10×5=200 JE_p = mgh = 4 \times 10 \times 5 = 200\text{ J} is completely converted into kinetic energy EkE_k just before impact, making 200 J200\text{ J} the correct answer.

Step-by-Step Solution

1
Calculate the initial potential energy at maximum height
Ep=mgh=4 kg×10 m s2×5 m=200 JE_p = mgh = 4\text{ kg} \times 10\text{ m s}^{-2} \times 5\text{ m} = 200\text{ J}
At the top of the fall, all mechanical energy is stored as gravitational potential energy.
2
Apply the principle of conservation of mechanical energy
Ek=Ep=200 JE_k = E_p = 200\text{ J}
In the absence of resistive forces such as air drag, potential energy lost converts completely into kinetic energy gained.

Key Concept

Conservation of Mechanical Energy
Estimated Time:45s
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