Here are the solutions to the questions:
QUESTION 3: ROTATIONAL MOTION
3.1.1 Calculate the angular acceleration of the flywheel.
Step 1: Convert initial and final angular speeds from revolutions per minute (r/min) to radians per second (rad/s).
ωi=200r/min×1rev2πrad×60s1min=60400πrad/s=320πrad/s
ωf=720r/min×1rev2πrad×60s1min=601440πrad/s=24πrad/s
Step 2: Calculate the angular acceleration α using the formula α=tωf−ωi.
α=8s24πrad/s−320πrad/s
α=8372π−20πrad/s2=2452πrad/s2=613πrad/s2
α≈6.81rad/s2
The angular acceleration is 613πrad/s2or6.81rad/s2.
3.1.2 Determine the number of revolutions made during the 8 s.
Step 1: Calculate the angular displacement Δθ using the formula Δθ=2(ωi+ωf)t.
Δθ=2(320πrad/s+24πrad/s)×8s
Δθ=2(320π+72π)×8rad=692π×8rad=346π×8rad=3368πrad
Step 2: Convert the angular displacement from radians to revolutions.
Numberofrevolutions=2πrad/revΔθ=2πrad/rev3368πrad=6368rev=3184rev
Numberofrevolutions≈61.33rev
The number of revolutions made is 3184revolutionsor61.33revolutions.
3.2.1 Calculate the torque required on the drum to lift the load.
Step 1: Calculate the radius of the drum and the force required to lift the load.
Diameter D=380mm=0.380 m
Radius r=2D=20.380m=0.190 m
Mass m=1250 kg
Force (weight) F=mg=1250kg×9.8m/s2=12250 N
Step 2: Calculate the torque τ using the formula τ=Fr.
τ=12250N×0.190m=2327.5N\cdotm
The torque required is 2327.5N\cdotm.
3.2.2 If the drum rotates at 24 r/min, calculate the power developed.
Step 1: Convert the angular speed from r/min to rad/s.
ω=24r/min×1rev2πrad×60s1min=6048πrad/s=54πrad/s
Step 2: Calculate the power developed P using the formula P=τω.
P=2327.5N\cdotm×54πrad/s
P=1862πW≈5850.7W
The power developed is 1862πWor5850.7W.
QUESTION 4: DYNAMICS
4.1.1 Calculate the kinetic energy of the bakkie.
Step 1: Convert the speed from kilometers per hour (km/h) to meters per second (m/s).
v=90km/h×1km1000m×3600s1h=25m/s
Step 2: Calculate the kinetic energy KE using the formula KE=21mv2.
KE=21×1800kg×(25m/s)2
KE=900kg×625m2/s2=562500J
The kinetic energy is 562500J.
4.1.2 If the bakkie is brought to rest in 40 m, calculate the average braking force.
Step 1: Use the work-energy theorem, W=ΔKE.
The initial kinetic energy KEi=562500 J (from 4.1.1).
The final kinetic energy KEf=0 J (since the bakkie comes to rest).
W=KEf−KEi=0−562500J=−562500J
Step 2: Calculate the average braking force Fb using W=Fbdcosθ.
The braking force acts opposite to the direction of motion, so θ=180∘ and cos(180∘)=−1.
−562500J=Fb×40m×(−1)
Fb=40m562500J=14062.5N
The average braking force is 14062.5N.
4.2.1 Calculate the tension in the rope.
Step 1: Identify the forces acting on the crate and apply Newton's second law.
Mass m=50 kg
Acceleration a=1.2m/s2 (upwards)
Gravitational acceleration g=9.8m/s2
The forces are tension T (upwards) and weight mg (downwards).
∑Fy=may⟹T−mg=ma
T=m(g+a)
Step 2: Substitute the values and calculate the tension.
T=50kg×(9.8m/s2+1.2m/s2)
T=50kg×11.0m/s2=550N
The tension in the rope is 550N.
4.2.2 Calculate the work done in lifting the crate.
Step 1: Use the formula for work done by a constant force, W=Fdcosθ.
The force doing the work is the tension T=550 N (from 4.2.1).
The distance d=30 m.
The force and displacement are in the same direction, so θ=0∘ and cos(0∘)=1.
W=Td
Step 2: Substitute the values and calculate the work done.
W=550N×30m=16500J
The work done in lifting the crate is 16500J.
4.3.1 Calculate the maximum static frictional force acting on the box.
Step 1: Calculate the normal force N acting on the box.
Mass m=25 kg
Angle of inclination θ=25∘
Normal force N=mgcosθ
N=25kg×9.8m/s2×cos(25∘)
N=245N×0.9063≈222.04N
Step 2: Calculate the maximum static frictional force fs,max using the formula fs,max=μsN.
Coefficient of static friction μs=0.35
fs,max=0.35×222.04N≈77.71N
The maximum static frictional force is 77.71N.
4.3.2 Show that the box is indeed about to slide down the plane.
Step 1: Calculate the component of the gravitational force parallel to the incline, which tends to pull the box down.
Fparallel=mgsinθ
Fparallel=25kg×9.8m/s2×sin(25∘)
Fparallel=245N×0.4226≈103.54N
Step 2: Compare the parallel component of gravity with the maximum static frictional force.
From 4.3.1, the maximum static frictional force fs,max=77.71 N.
The component of gravity pulling the box down the incline is Fparallel=103.54 N.
Since Fparallel(103.54N)>fs,max(77.71N), the force pulling the box down the incline is greater than the maximum static friction that can oppose it. This means the box will overcome static friction and slide down the plane, confirming that it is indeed in a state where it will slide.
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