Mechanics

227 questions

Question 61Question

A boat moves due north across a river at a speed of 4.0 m s14.0\text{ m s}^{-1} relative to the water. If the river current flows due east at a speed of 3.0 m s13.0\text{ m s}^{-1}, what is the magnitude of the resultant velocity of the boat relative to the riverbank?

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Answer: 5.0 m s15.0\text{ m s}^{-1}

Answer

The magnitude of the resultant velocity of the boat relative to the riverbank is 5.0 m s15.0\text{ m s}^{-1}.
The resultant velocity magnitude is found by applying vector addition for perpendicular components: vresultant=(4.0)2+(3.0)2=25.0=5.0 m s1v_{resultant} = \sqrt{(4.0)^2 + (3.0)^2} = \sqrt{25.0} = 5.0\text{ m s}^{-1}.

Step-by-Step Solution

1
Identify the given velocity components and their directions
Northward velocity component vy=4.0 m s1v_y = 4.0\text{ m s}^{-1}, Eastward velocity component vx=3.0 m s1v_x = 3.0\text{ m s}^{-1}.
The motion of the boat and the movement of the river current act in perpendicular directions (9090^\circ to each other).
2
Calculate the resultant magnitude using vector addition (Pythagorean theorem)
v=vx2+vy2=(3.0)2+(4.0)2=9.0+16.0=25.0=5.0 m s1v = \sqrt{v_x^2 + v_y^2} = \sqrt{(3.0)^2 + (4.0)^2} = \sqrt{9.0 + 16.0} = \sqrt{25.0} = 5.0\text{ m s}^{-1}.
For two orthogonal vectors, the magnitude of the vector sum equals the hypotenuse of the right triangle formed by the vector components.

Key Concept

Vector Addition of Perpendicular Quantities
Estimated Time:1m 0s
Question 62Question

A horizontal jet of water issuing from a nozzle with a cross-sectional area of 2.0×103 m22.0 \times 10^{-3}\text{ m}^2 at a speed of 20 m s120\text{ m s}^{-1} strikes a vertical wall perpendicularly. If the water rebounds horizontally in the opposite direction at a speed of 5.0 m s15.0\text{ m s}^{-1}, what is the magnitude of the force exerted by the water stream on the wall? (Density of water = 1000 kg m31000\text{ kg m}^{-3})

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Answer: 1000 N1000\text{ N}

Answer

The magnitude of the force exerted by the water jet on the wall is 1000 N1000\text{ N}.
According to Newton's second law, force is the rate of change of linear momentum. The mass of water hitting the wall each second is ΔmΔt=ρAv1=1000×2.0×103×20=40 kg s1\frac{\Delta m}{\Delta t} = \rho A v_1 = 1000 \times 2.0 \times 10^{-3} \times 20 = 40\text{ kg s}^{-1}. Taking the initial direction as positive (+20 m s1+20\text{ m s}^{-1}), the rebounding velocity is opposite in direction (5.0 m s1-5.0\text{ m s}^{-1}). The magnitude of the change in velocity is 5.020=25 m s1|-5.0 - 20| = 25\text{ m s}^{-1}. Multiplying mass flow rate by the change in velocity gives a force magnitude of 40×25=1000 N40 \times 25 = 1000\text{ N}.

Step-by-Step Solution

1
Calculate the mass of water striking the wall per second (mass flow rate, ΔmΔt\frac{\Delta m}{\Delta t}).
ΔmΔt=ρAv1=1000 kg m3×(2.0×103 m2)×20 m s1=40 kg s1\frac{\Delta m}{\Delta t} = \rho A v_1 = 1000\text{ kg m}^{-3} \times (2.0 \times 10^{-3}\text{ m}^2) \times 20\text{ m s}^{-1} = 40\text{ kg s}^{-1}.
The volume of water reaching the wall per second is given by the cross-sectional area multiplied by its initial speed.
2
Determine the change in velocity vector per unit mass of water (Δv)(\Delta v).
Taking the direction towards the wall as positive, v1=+20 m s1v_1 = +20\text{ m s}^{-1} and v2=5.0 m s1v_2 = -5.0\text{ m s}^{-1}. Thus, Δv=v2v1=5.020=25.0 m s1\Delta v = v_2 - v_1 = -5.0 - 20 = -25.0\text{ m s}^{-1}.
Velocity is a vector quantity; rebounding in the opposite direction requires assigning opposite signs to the initial and final velocities.
3
Apply Newton's Second Law (F=ΔpΔtF = \frac{\Delta p}{\Delta t}) to find the magnitude of force on the wall.
F=ΔmΔtΔv=40 kg s1×25.0 m s1=1000 NF = \frac{\Delta m}{\Delta t} |\Delta v| = 40\text{ kg s}^{-1} \times 25.0\text{ m s}^{-1} = 1000\text{ N}.
By Newton's third law, the magnitude of force exerted on the wall equals the rate of change of momentum of the water stream.

Key Concept

Newton's Second Law and Linear Momentum Rate of Change
Question 63Question

A solid block of mass 0.60 kg0.60\text{ kg} and density 600 kg/m3600\text{ kg/m}^3 is held fully submerged in water of density 1000 kg/m31000\text{ kg/m}^3 by a light vertical string attached to the bottom of a container. What is the tension in the string? (Take g=10 m/s2g = 10\text{ m/s}^2)

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Answer: 4.0 N4.0\text{ N}

Answer

The tension in the string is 4.0 N4.0\text{ N}.
First, the volume of the block is computed as V=mρ=0.60600=1.0×103 m3V = \frac{m}{\rho} = \frac{0.60}{600} = 1.0 \times 10^{-3}\text{ m}^3. According to Archimedes' principle, the upthrust exerted by the displaced water is U=ρwaterVg=1000×1.0×103×10=10.0 NU = \rho_{\text{water}} V g = 1000 \times 1.0 \times 10^{-3} \times 10 = 10.0\text{ N}. The weight of the block is W=mg=0.60×10=6.0 NW = mg = 0.60 \times 10 = 6.0\text{ N}. For the block to remain completely submerged in equilibrium, the upward upthrust must balance the downward forces (the weight of the block and the tension TT pulling downward). Thus, T=UW=10.0 N6.0 N=4.0 NT = U - W = 10.0\text{ N} - 6.0\text{ N} = 4.0\text{ N}.

Step-by-Step Solution

1
Calculate the volume of the block using its mass and density.
V=mρblock=0.60 kg600 kg/m3=1.0×103 m3V = \frac{m}{\rho_{\text{block}}} = \frac{0.60\text{ kg}}{600\text{ kg/m}^3} = 1.0 \times 10^{-3}\text{ m}^3
The volume of fluid displaced equals the total volume of the fully submerged block.
2
Calculate the upward upthrust force exerted by the water.
U=ρwaterVg=1000 kg/m3×1.0×103 m3×10 m/s2=10.0 NU = \rho_{\text{water}} \cdot V \cdot g = 1000\text{ kg/m}^3 \times 1.0 \times 10^{-3}\text{ m}^3 \times 10\text{ m/s}^2 = 10.0\text{ N}
Archimedes' principle states upthrust equals the weight of the displaced fluid.
3
Calculate the downward gravitational weight of the block.
W=mg=0.60 kg×10 m/s2=6.0 NW = m \cdot g = 0.60\text{ kg} \times 10\text{ m/s}^2 = 6.0\text{ N}
Weight is the force exerted on the mass of the block by gravity.
4
Apply vertical force equilibrium to solve for string tension.
U=W+TT=UW=10.0 N6.0 N=4.0 NU = W + T \Rightarrow T = U - W = 10.0\text{ N} - 6.0\text{ N} = 4.0\text{ N}
The string is tied to the bottom, so tension acts downward to hold the buoyant block in equilibrium.

Key Concept

Archimedes' Principle and Static Equilibrium of Submerged Bodies
Question 64Question

An inclined plane of length 5 m5\text{ m} is used to lift a load of 400 N400\text{ N} through a vertical height of 1 m1\text{ m}. If an effort of 100 N100\text{ N} is applied parallel to the incline, what is the efficiency of the machine?

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Answer: 80%80\%

Answer

The efficiency of the machine is 80%80\%.
The correct answer of 80%80\% is obtained by finding the velocity ratio (distance moved by effort divided by distance moved by load, 5/1=55 / 1 = 5) and the mechanical advantage (load divided by effort, 400/100=4400 / 100 = 4), then calculating efficiency as (MA/VR)×100%=(4/5)×100%=80%(\text{MA} / \text{VR}) \times 100\% = (4 / 5) \times 100\% = 80\%.

Step-by-Step Solution

1
Calculate the Velocity Ratio (VR) of the inclined plane
VR=Length of inclineHeight=5 m1 m=5\text{VR} = \frac{\text{Length of incline}}{\text{Height}} = \frac{5\text{ m}}{1\text{ m}} = 5
Velocity Ratio is the distance moved by the effort divided by the distance moved by the load.
2
Calculate the Mechanical Advantage (MA)
MA=LoadEffort=400 N100 N=4\text{MA} = \frac{\text{Load}}{\text{Effort}} = \frac{400\text{ N}}{100\text{ N}} = 4
Mechanical Advantage measures how many times a machine multiplies the applied force.
3
Calculate the Efficiency
Efficiency=(MAVR)×100%=(45)×100%=80%\text{Efficiency} = \left(\frac{\text{MA}}{\text{VR}}\right) \times 100\% = \left(\frac{4}{5}\right) \times 100\% = 80\%
Efficiency is defined as the ratio of Mechanical Advantage to Velocity Ratio expressed as a percentage.

Key Concept

Efficiency of Simple Machines (Inclined Plane)
Estimated Time:45s
Question 65Question

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 66Question

A crate on a smooth surface is simultaneously pulled by two horizontal forces. One force of magnitude 9.0 N9.0\text{ N} acts towards the East, and another force of magnitude 12.0 N12.0\text{ N} acts towards the North. What is the magnitude of the resultant force acting on the crate in newtons?

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Answer: 15

Answer

The magnitude of the resultant force acting on the crate is 15.0 N15.0\text{ N}.
Because the two pulling forces are perpendicular, their resultant magnitude is calculated using vector addition via the Pythagorean theorem: R=9.02+12.02=15.0 NR = \sqrt{9.0^2 + 12.0^2} = 15.0\text{ N}.

Step-by-Step Solution

1
Determine the angle between the two given vectors
The forces are perpendicular (9090^\circ).
East and North cardinal directions are orthogonal to each other.
2
Compute the resultant magnitude using vector synthesis
R=9.02+12.02=81+144=225=15.0 NR = \sqrt{9.0^2 + 12.0^2} = \sqrt{81 + 144} = \sqrt{225} = 15.0\text{ N}
For perpendicular force vectors, the resultant magnitude is the hypotenuse of the right triangle formed by the vector components.

Key Concept

Vector addition of perpendicular forces using the Pythagorean theorem
Estimated Time:1m 15s
Question 67Question

A solid sphere of mass 0.40 kg0.40\text{ kg} and relative density 2.52.5 is held fully submerged in a liquid of density 800 kg/m3800\text{ kg/m}^3 by a light string attached to a fixed support. What is the tension in the string? (Take g=10 m/s2g = 10\text{ m/s}^2)

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Answer: 2.72 N2.72\text{ N}

Answer

The tension in the string is 2.72 N2.72\text{ N}.
The sphere has a weight of 4.0 N4.0\text{ N} acting downward. When fully submerged, it displaces a volume of liquid equal to its own volume (1.6×104 m31.6 \times 10^{-4}\text{ m}^3). The displaced liquid of density 800 kg/m3800\text{ kg/m}^3 exerts an upward buoyant force (upthrust) of 1.28 N1.28\text{ N}. Tension balances the remaining downward force: T=4.0 N1.28 N=2.72 NT = 4.0\text{ N} - 1.28\text{ N} = 2.72\text{ N}.

Step-by-Step Solution

1
Calculate the weight of the sphere
W=mg=0.40 kg×10 m/s2=4.0 NW = mg = 0.40\text{ kg} \times 10\text{ m/s}^2 = 4.0\text{ N}
The force of gravity acting downward on the mass.
2
Determine the volume of the sphere using its relative density
Density of sphere ρs=2.5×1000 kg/m3=2500 kg/m3\rho_s = 2.5 \times 1000\text{ kg/m}^3 = 2500\text{ kg/m}^3. Volume V=mρs=0.402500=1.6×104 m3V = \frac{m}{\rho_s} = \frac{0.40}{2500} = 1.6 \times 10^{-4}\text{ m}^3.
Relative density is the ratio of the substance's density to the density of water (1000 kg/m31000\text{ kg/m}^3).
3
Calculate the upthrust exerted by the liquid
U=Vρliquidg=(1.6×104)×800×10=1.28 NU = V \cdot \rho_{\text{liquid}} \cdot g = (1.6 \times 10^{-4}) \times 800 \times 10 = 1.28\text{ N}
By Archimedes' principle, upthrust equals the weight of the fluid displaced by the submerged volume.
4
Calculate tension in the string
T=WU=4.0 N1.28 N=2.72 NT = W - U = 4.0\text{ N} - 1.28\text{ N} = 2.72\text{ N}
For vertical equilibrium of the submerged body, weight acts downward while upthrust and tension act upward.

Key Concept

Archimedes' Principle and Apparent Weight
Estimated Time:1m 30s
Question 68Question

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 69Question

A uniform metre rule of mass 120 g120\text{ g} is balanced horizontally on a pivot placed at the 40 cm40\text{ cm} mark when an unknown mass mm is suspended at the 10 cm10\text{ cm} mark. What is the value of the mass mm in grams?

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Answer: 40

Answer

The mass mm required to balance the metre rule horizontally is 40 g40\text{ g}.
According to the Principle of Moments, a system is in rotational equilibrium when the sum of anticlockwise moments equals the sum of clockwise moments about the pivot. The weight of the 120 g120\text{ g} uniform metre rule acts at its center of gravity (50 cm50\text{ cm} mark), which is 10 cm10\text{ cm} to the right of the pivot at 40 cm40\text{ cm}. This creates a clockwise moment of 120 g×10 cm=1200 gcm120\text{ g} \times 10\text{ cm} = 1200\text{ g}\cdot\text{cm}. The mass mm is suspended at the 10 cm10\text{ cm} mark, which is 30 cm30\text{ cm} to the left of the pivot, creating an anticlockwise moment of m×30 cmm \times 30\text{ cm}. Setting 30m=120030m = 1200 yields m=40 gm = 40\text{ g}.

Step-by-Step Solution

1
Determine the position of the center of gravity of the metre rule.
Center of gravity is at the 50 cm50\text{ cm} mark.
A uniform metre rule has its weight concentrated at its geometric midpoint.
2
Calculate perpendicular distances from the pivot at 40 cm40\text{ cm} to all acting forces.
Distance to rule weight = 50 cm40 cm=10 cm50\text{ cm} - 40\text{ cm} = 10\text{ cm}; Distance to mass mm = 40 cm10 cm=30 cm40\text{ cm} - 10\text{ cm} = 30\text{ cm}.
Moments are calculated by multiplying force (or mass) by perpendicular distance from the turning point.
3
Apply the Principle of Moments for equilibrium.
Sum of anticlockwise moments = Sum of clockwise moments     m×30=120×10\implies m \times 30 = 120 \times 10.
For rotational equilibrium, the total clockwise moment must equal the total anticlockwise moment about the pivot.
4
Solve for the unknown mass mm.
m=40 gm = 40\text{ g}.
Dividing 1200 gcm1200\text{ g}\cdot\text{cm} by 30 cm30\text{ cm} gives 40 g40\text{ g}.

Key Concept

Principle of Moments and Center of Gravity of a Uniform Body
Estimated Time:50s
Question 70Question

A rigid rod ABAB of length 2.0 m2.0\text{ m} is hinged at end AA. A force of 50 N50\text{ N} is applied at end BB at an angle of 3030^\circ to the rod. What is the moment of this force about the hinge AA?

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Answer: 50 N m50\text{ N m}

Answer

The moment of the force about hinge AA is 50 N m50\text{ N m}.
The moment of a force about a pivot is calculated by multiplying the force magnitude by the perpendicular distance to the pivot line of action (F×LsinθF \times L \sin\theta). Substituting F=50 NF = 50\text{ N}, L=2.0 mL = 2.0\text{ m}, and sin(30)=0.5\sin(30^\circ) = 0.5 gives 50×2.0×0.5=50 N m50 \times 2.0 \times 0.5 = 50\text{ N m}.

Step-by-Step Solution

1
Identify the formula for the moment of a force applied at an angle.
Moment=F×d=F×Lsinθ\text{Moment} = F \times d_\perp = F \times L \sin\theta
Moment is defined as the product of the magnitude of the force and the perpendicular distance from the line of action of the force to the pivot point.
2
Substitute the given values into the formula.
Moment=50 N×2.0 m×sin(30)\text{Moment} = 50\text{ N} \times 2.0\text{ m} \times \sin(30^\circ)
The force F=50 NF = 50\text{ N}, distance L=2.0 mL = 2.0\text{ m}, and angle θ=30\theta = 30^\circ.
3
Calculate the final moment value.
Moment=50×2.0×0.5=50 N m\text{Moment} = 50 \times 2.0 \times 0.5 = 50\text{ N m}
Since sin(30)=0.5\sin(30^\circ) = 0.5, the perpendicular distance is 1.0 m1.0\text{ m}, giving a moment of 50 N m50\text{ N m}.

Key Concept

Moment of a Force at an Angle
Estimated Time:45s
Question 71Question

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 72Question

A car initially traveling at a constant speed of 15 m/s15\text{ m/s} accelerates uniformly at 2 m/s22\text{ m/s}^2 for 5 s5\text{ s}. It then maintains the acquired maximum speed for 10 s10\text{ s} before coming to rest under uniform retardation in 4 s4\text{ s}. What is the total distance covered by the car during the entire motion?

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Answer: 400

Answer

The total distance covered by the car during the entire motion is 400 m400\text{ m}.
The total distance is calculated by summing the distances covered in the three distinct phases of motion: acceleration (100 m100\text{ m}), uniform velocity (250 m250\text{ m}), and uniform retardation (50 m50\text{ m}), yielding a total distance of 400 m400\text{ m}.

Step-by-Step Solution

1
Calculate final speed and distance for the acceleration phase.
Final speed v=25 m/sv = 25\text{ m/s} and distance s1=100 ms_1 = 100\text{ m}.
Using kinematic equations v=u+at1=15+(2)(5)=25 m/sv = u + a t_1 = 15 + (2)(5) = 25\text{ m/s} and s1=ut1+12at12=15(5)+12(2)(52)=75+25=100 ms_1 = u t_1 + \frac{1}{2}a t_1^2 = 15(5) + \frac{1}{2}(2)(5^2) = 75 + 25 = 100\text{ m}.
2
Calculate the distance covered during the constant speed phase.
Distance s2=250 ms_2 = 250\text{ m}.
The car maintains the acquired speed of 25 m/s25\text{ m/s} for 10 s10\text{ s}, giving s2=vt2=25×10=250 ms_2 = v \cdot t_2 = 25 \times 10 = 250\text{ m}.
3
Calculate the distance covered during the retardation phase.
Distance s3=50 ms_3 = 50\text{ m}.
Using average velocity for uniform retardation to rest: s3=v+02t3=252×4=50 ms_3 = \frac{v + 0}{2} t_3 = \frac{25}{2} \times 4 = 50\text{ m}.
4
Sum the distances from all three stages to determine total distance.
Total distance S=400 mS = 400\text{ m}.
S=s1+s2+s3=100+250+50=400 mS = s_1 + s_2 + s_3 = 100 + 250 + 50 = 400\text{ m}.

Key Concept

Multi-stage linear motion and equations of uniform acceleration
Question 73Question

A wheel and axle machine having a wheel radius of 25 cm25\text{ cm} and an axle radius of 5 cm5\text{ cm} is used to raise a load of mass 80 kg80\text{ kg} vertically through a height of 10 m10\text{ m}. If the efficiency of the machine is 80%80\%, what is the work done against friction during this operation? (Take g=10 m s2g = 10\text{ m s}^{-2})

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Answer: 2,000 J2,000\text{ J}

Answer

2,000 J2,000\text{ J}
The useful work done on the load is Wout=mgh=80×10×10=8000 JW_{\text{out}} = mgh = 80 \times 10 \times 10 = 8000\text{ J}. Since efficiency is 80%80\%, the total work input required is Win=80000.80=10,000 JW_{\text{in}} = \frac{8000}{0.80} = 10,000\text{ J}. Therefore, the work lost to friction is WinWout=10,000 J8,000 J=2,000 JW_{\text{in}} - W_{\text{out}} = 10,000\text{ J} - 8,000\text{ J} = 2,000\text{ J}.

Step-by-Step Solution

1
Calculate the useful work output of the machine
Wout=mgh=80 kg×10 m s2×10 m=8,000 JW_{\text{out}} = mgh = 80\text{ kg} \times 10\text{ m s}^{-2} \times 10\text{ m} = 8,000\text{ J}
Useful work output is the gravitational potential energy gained by raising the load.
2
Calculate the total work input using the efficiency equation
Win=WoutEfficiency=8,000 J0.80=10,000 JW_{\text{in}} = \frac{W_{\text{out}}}{\text{Efficiency}} = \frac{8,000\text{ J}}{0.80} = 10,000\text{ J}
Efficiency is defined as Work OutputWork Input\frac{\text{Work Output}}{\text{Work Input}}, so Work Input = Work OutputEfficiency\frac{\text{Work Output}}{\text{Efficiency}}.
3
Determine the work done against friction
Wfriction=WinWout=10,000 J8,000 J=2,000 JW_{\text{friction}} = W_{\text{in}} - W_{\text{out}} = 10,000\text{ J} - 8,000\text{ J} = 2,000\text{ J}
The energy wasted as heat and friction is the difference between total work input and useful work output.

Key Concept

Efficiency of Simple Machines and Work Done Against Friction
Question 74Question

A traffic officer on a stationary motorcycle spots a car passing at a constant speed of 15 m/s15\text{ m/s}. The officer immediately pursues the car, accelerating uniformly from rest at 4 m/s24\text{ m/s}^2 for 5 s5\text{ s}, after which the motorcycle continues at the constant speed attained. How long after setting off does the motorcycle overtake the car?

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Answer: 10 s10\text{ s}

Answer

The total time required for the motorcycle to overtake the car is 10 s10\text{ s}.
During the first 5 s5\text{ s}, the motorcycle accelerates from rest at 4 m/s24\text{ m/s}^2 to 20 m/s20\text{ m/s}, covering 50 m50\text{ m}. In that same interval, the car moving at 15 m/s15\text{ m/s} covers 75 m75\text{ m}, creating a 25 m25\text{ m} separation gap. Beyond 5 s5\text{ s}, the motorcycle maintains 20 m/s20\text{ m/s} and closes in on the car (15 m/s15\text{ m/s}) at a relative speed of 5 m/s5\text{ m/s}. It takes 5 s5\text{ s} to close the 25 m25\text{ m} gap, making the total pursuit time 10 s10\text{ s}.

Step-by-Step Solution

1
Calculate the state of both vehicles at the end of the motorcycle's acceleration phase (t1=5 st_1 = 5\text{ s}).
Motorcycle speed v=u+at=0+4(5)=20 m/sv = u + at = 0 + 4(5) = 20\text{ m/s}. Motorcycle distance s1=12at2=12(4)(52)=50 ms_1 = \frac{1}{2} a t^2 = \frac{1}{2}(4)(5^2) = 50\text{ m}. Car distance scar=vcar×t=15×5=75 ms_{\text{car}} = v_{\text{car}} \times t = 15 \times 5 = 75\text{ m}.
Determine the position gap and relative speed after the acceleration phase ends.
2
Determine the remaining distance gap and relative speed between the vehicles.
Separation gap d=75 m50 m=25 md = 75\text{ m} - 50\text{ m} = 25\text{ m}. Relative speed vrel=20 m/s15 m/s=5 m/sv_{\text{rel}} = 20\text{ m/s} - 15\text{ m/s} = 5\text{ m/s}.
Both vehicles now move at constant velocities, so relative speed determines how quickly the gap closes.
3
Calculate the time taken in the second phase and sum for total time.
Phase 2 time t2=dvrel=255=5 st_2 = \frac{d}{v_{\text{rel}}} = \frac{25}{5} = 5\text{ s}. Total time t=t1+t2=5 s+5 s=10 st = t_1 + t_2 = 5\text{ s} + 5\text{ s} = 10\text{ s}.
The total duration of pursuit is the acceleration duration plus the constant velocity catch-up duration.

Key Concept

Multi-stage linear motion involving uniform acceleration followed by constant velocity.
Estimated Time:1m 30s
Question 75Question

A ball of mass 0.20 kg0.20\text{ kg} moving horizontally towards a vertical wall at a speed of 15 m s115\text{ m s}^{-1} rebounds in the opposite direction at 10 m s110\text{ m s}^{-1}. If the impact with the wall lasts for 0.020 s0.020\text{ s}, what is the magnitude of the average force exerted on the ball by the wall?

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Answer: 250 N250\text{ N}

Answer

The magnitude of the average force exerted on the ball by the wall is 250 N250\text{ N}.
The average force is determined by Newton's second law (F=ΔpΔtF = \frac{\Delta p}{\Delta t}). Because the ball rebounds in the opposite direction, velocity changes from +15 m s1+15\text{ m s}^{-1} to 10 m s1-10\text{ m s}^{-1}, yielding a total velocity change magnitude of 25 m s125\text{ m s}^{-1}. Multiplying by mass (0.20 kg0.20\text{ kg}) gives an impulse magnitude of 5.0 N s5.0\text{ N s}. Dividing impulse by the contact time (0.020 s0.020\text{ s}) yields 250 N250\text{ N}.

Step-by-Step Solution

1
Establish vector direction and assign initial and final velocities
Initial velocity u=+15 m s1u = +15\text{ m s}^{-1}, final velocity v=10 m s1v = -10\text{ m s}^{-1}
Velocity is a vector quantity, so reversing direction requires a opposite sign convention.
2
Calculate the change in momentum (impulse)
\Delta p = m(v - u) = 0.20 \times (-10 - 15) = 0.20 \times (-25) = -5.0\text{ N s}
Impulse is equal to the change in linear momentum.
3
Calculate the magnitude of the average force
F = \frac{|\Delta p|}{\Delta t} = \frac{5.0\text{ N s}}{0.020\text{ s}} = 250\text{ N}
By Newton's second law, average force equals rate of change of momentum (F = \Delta p / \Delta t).

Key Concept

Impulse-Momentum Theorem and Vector Nature of Momentum
Estimated Time:1m 0s
Question 76Question

A cannonball is fired from ground level with an initial speed of 50 m/s50\text{ m/s} at an angle θ\theta above the horizontal such that tanθ=43\tan \theta = \frac{4}{3}. Assuming acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2 and neglecting air resistance, what is the magnitude of the velocity of the cannonball at the highest point of its trajectory?

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Answer: 30 m/s30\text{ m/s}

Answer

30 m/s30\text{ m/s}
At the maximum height of a projectile's flight, the vertical velocity component drops to zero due to gravity, while the horizontal component remains unchanged because horizontal acceleration is zero. For a launch speed of 50 m/s50\text{ m/s} at an angle with tanθ=43\tan \theta = \frac{4}{3}, cosθ=35\cos \theta = \frac{3}{5}. The magnitude of the velocity at apex is therefore equal to ux=50×35=30 m/su_x = 50 \times \frac{3}{5} = 30\text{ m/s}.

Step-by-Step Solution

1
Resolve the initial velocity vector into orthogonal horizontal and vertical components.
Given tanθ=43\tan \theta = \frac{4}{3}, the trigonometric ratios are cosθ=35\cos \theta = \frac{3}{5} and sinθ=45\sin \theta = \frac{4}{5}. Thus, ux=50×35=30 m/su_x = 50 \times \frac{3}{5} = 30\text{ m/s} and uy=50×45=40 m/su_y = 50 \times \frac{4}{5} = 40\text{ m/s}.
Resolving 2D projectile motion into independent orthogonal components simplifies kinematic analysis.
2
Determine the velocity components at the apex (highest point) of the trajectory.
At maximum height, the vertical velocity component vy=0 m/sv_y = 0\text{ m/s}. Since there is no horizontal acceleration, the horizontal velocity component remains vx=ux=30 m/sv_x = u_x = 30\text{ m/s}.
Gravity acts purely vertically, reducing vertical velocity to zero at the apex while leaving horizontal velocity unchanged.
3
Calculate the magnitude of total velocity at maximum height.
v=vx2+vy2=302+02=30 m/sv = \sqrt{v_x^2 + v_y^2} = \sqrt{30^2 + 0^2} = 30\text{ m/s}.
The magnitude of a 2D velocity vector is determined by combining its orthogonal components using the Pythagorean formula.

Key Concept

Velocity components at maximum height in projectile motion
Question 77Question

A stone is thrown vertically downwards from the top of a 60 m60\text{ m} high tower with an initial speed of 5 m/s5\text{ m/s}. Taking acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, calculate the time taken, in seconds, for the stone to reach the ground.

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Answer: 3

Answer

The stone takes 3 s3\text{ s} to reach the ground.
Applying the equation h=ut+12gt2h = ut + \frac{1}{2}gt^2 with h=60 mh = 60\text{ m}, u=5 m/su = 5\text{ m/s}, and g=10 m/s2g = 10\text{ m/s}^2 yields 60=5t+5t260 = 5t + 5t^2. Dividing by 55 gives t2+t12=0t^2 + t - 12 = 0, which factorizes into (t+4)(t3)=0(t + 4)(t - 3) = 0. Rejecting t=4 st = -4\text{ s} leaves the correct time of 3 s3\text{ s}.

Step-by-Step Solution

1
Set up the vertical motion equation
Using h=ut+12gt2h = ut + \frac{1}{2}gt^2, substitute h=60 mh = 60\text{ m}, u=5 m/su = 5\text{ m/s}, and g=10 m/s2g = 10\text{ m/s}^2.
This equation directly relates displacement, initial speed, acceleration, and time.
2
Form and solve the quadratic equation for time
60=5t+5t2t2+t12=0(t3)(t+4)=060 = 5t + 5t^2 \Rightarrow t^2 + t - 12 = 0 \Rightarrow (t - 3)(t + 4) = 0, giving t=3 st = 3\text{ s}.
Time must be positive, so the physically meaningful solution is t=3 st = 3\text{ s}.

Key Concept

Vertical motion under gravity with non-zero initial downward velocity
Question 78Question

A projectile is launched from horizontal ground with an initial speed of 60 m/s60\text{ m/s} at an angle of 6060^\circ to the horizontal. Taking g=10 m/s2g = 10\text{ m/s}^2 and neglecting air resistance, what is the speed of the projectile at its maximum height?

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Answer: 30 m/s30\text{ m/s}

Answer

The speed of the projectile at its maximum height is 30 m/s30\text{ m/s}.
In two-dimensional projectile motion, gravity acts purely in the vertical direction. At the apex (maximum height), the vertical velocity component vyv_y drops to zero. However, the horizontal velocity component vx=ucosθv_x = u \cos \theta remains constant throughout the entire flight because air resistance is neglected. Consequently, the speed at maximum height equals ucos60=60×0.5=30 m/su \cos 60^\circ = 60 \times 0.5 = 30\text{ m/s}.

Step-by-Step Solution

1
Resolve initial launch velocity into orthogonal horizontal and vertical components.
ux=ucosθ=60cos60=30 m/su_x = u \cos \theta = 60 \cos 60^\circ = 30\text{ m/s} and uy=usinθ=60sin60=303 m/su_y = u \sin \theta = 60 \sin 60^\circ = 30\sqrt{3}\text{ m/s}.
Projectile motion consists of independent horizontal and vertical motions.
2
Determine the velocity components at the apex (maximum height).
At the peak, vertical velocity vy=0 m/sv_y = 0\text{ m/s} while horizontal velocity remains vx=ux=30 m/sv_x = u_x = 30\text{ m/s}.
Gravity acts vertically causing vyv_y to become zero at peak height, whereas no horizontal force acts, leaving vxv_x unchanged.
3
Calculate the magnitude of total velocity (speed) at maximum height.
v=vx2+vy2=302+02=30 m/sv = \sqrt{v_x^2 + v_y^2} = \sqrt{30^2 + 0^2} = 30\text{ m/s}.
Speed is the resultant magnitude of orthogonal velocity components.

Key Concept

Velocity at Maximum Height in Projectile Motion
Question 79Question

A trolley of mass 0.40 kg0.40\text{ kg} moving to the right with a velocity of 5.0 m s15.0\text{ m s}^{-1} collides head-on with a second trolley of mass 0.60 kg0.60\text{ kg} moving to the left at 2.5 m s12.5\text{ m s}^{-1}. If the two trolleys stick together on impact, what is their combined velocity immediately after the collision?

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Answer: 0.50 m s10.50\text{ m s}^{-1} to the right

Answer

0.50 m s10.50\text{ m s}^{-1} to the right
By adopting a standard vector sign convention where movement to the right is positive and movement to the left is negative, the initial momentum is pi=(0.40 kg×5.0 m s1)+(0.60 kg×2.5 m s1)=2.01.5=0.50 kg m s1p_i = (0.40 \text{ kg} \times 5.0 \text{ m s}^{-1}) + (0.60 \text{ kg} \times -2.5 \text{ m s}^{-1}) = 2.0 - 1.5 = 0.50 \text{ kg m s}^{-1}. Because the trolleys stick together, their total mass becomes 0.40 kg+0.60 kg=1.0 kg0.40 \text{ kg} + 0.60 \text{ kg} = 1.0 \text{ kg}. Dividing the total momentum by the combined mass gives a final velocity of +0.50 m s1+0.50 \text{ m s}^{-1}, indicating movement to the right.

Step-by-Step Solution

1
Assign a directional sign convention for velocity vectors
Rightward velocity u1=+5.0 m s1u_1 = +5.0\text{ m s}^{-1}, Leftward velocity u2=2.5 m s1u_2 = -2.5\text{ m s}^{-1}
Linear momentum is a vector quantity, so direction must be accounted for using opposite algebraic signs.
2
Calculate total initial linear momentum of the system
pi=m1u1+m2u2=(0.40×5.0)+(0.60×(2.5))=2.01.5=+0.50 kg m s1p_i = m_1 u_1 + m_2 u_2 = (0.40 \times 5.0) + (0.60 \times (-2.5)) = 2.0 - 1.5 = +0.50\text{ kg m s}^{-1}
Sum the individual initial momenta of both trolleys.
3
Apply the principle of conservation of linear momentum to solve for final combined velocity
v=pim1+m2=+0.500.40+0.60=+0.50 m s1v = \frac{p_i}{m_1 + m_2} = \frac{+0.50}{0.40 + 0.60} = +0.50\text{ m s}^{-1}
Since no external net force acts on the system, total initial momentum equals total final momentum.

Key Concept

Conservation of Linear Momentum in Inelastic Collisions
Estimated Time:1m 30s
Question 80Question

A constant force of 12 N12\text{ N} acts for 4.0 s4.0\text{ s} on a body of mass 3.0 kg3.0\text{ kg} that is initially moving at 5.0 m s15.0\text{ m s}^{-1} in the direction opposite to the force. What is the final velocity of the body in the direction of the applied force?

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Answer: 11 m s111\text{ m s}^{-1}

Answer

The final velocity of the body in the direction of the force is 11 m s111\text{ m s}^{-1}.
By the impulse-momentum theorem, the impulse FΔt=12×4.0=48 N sF \Delta t = 12 \times 4.0 = 48\text{ N s} causes a velocity change Δv=483.0=16 m s1\Delta v = \frac{48}{3.0} = 16\text{ m s}^{-1} in the direction of the force. Since the body initially moved in the opposite direction at 5.0 m s1-5.0\text{ m s}^{-1}, the final velocity is 5.0+16=11 m s1-5.0 + 16 = 11\text{ m s}^{-1} in the direction of the force.

Step-by-Step Solution

1
Assign direction signs to physical quantities based on a chosen coordinate system.
Let the direction of the applied force be positive (+). Then F=+12 NF = +12\text{ N}, m=3.0 kgm = 3.0\text{ kg}, t=4.0 st = 4.0\text{ s}, and initial velocity u=5.0 m s1u = -5.0\text{ m s}^{-1}.
Velocity and force are vector quantities; motion opposite to the force must carry a negative sign.
2
Calculate the impulse delivered by the force.
Impulse=F×Δt=12 N×4.0 s=48 N s\text{Impulse} = F \times \Delta t = 12\text{ N} \times 4.0\text{ s} = 48\text{ N s}.
Impulse equals force multiplied by the time interval over which it acts.
3
Apply the impulse-momentum theorem FΔt=m(vu)F \Delta t = m(v - u) to solve for final velocity vv.
48=3.0×(v(5.0))    16=v+5.0    v=11 m s148 = 3.0 \times (v - (-5.0)) \implies 16 = v + 5.0 \implies v = 11\text{ m s}^{-1}.
The change in linear momentum of an object is equal to the net impulse applied to it.

Key Concept

Impulse-Momentum Theorem and Vector Sign Conventions
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