2008 June Exam Higher Grade Paper 1 Q 7
7.1 The Principle of Conservation of Momentum states that:
∗Thetotallinearmomentumofanisolatedsystemremainsconstantinbothmagnitudeanddirection.∗
7.2 Percy's statement is ∗FALSE∗.
Explanation: The system (Percy and the bike) is not isolated because an external frictional force acts on it, causing it to slow down and stop. Therefore, the total momentum of the system is not conserved. Percy kept moving forward due to inertia.
7.3 Step 1: Identify the given values.
Mass of Percy mP=75 kg
Mass of quad bike mQB=100 kg
Total mass of the system M=mP+mQB=75kg+100kg=175 kg
Initial velocity of the system u=20 m/s
Final velocity of the system v=0 m/s
Step 2: Calculate the change in momentum.
Δp=M(v−u)
Δp=(175kg)(0m/s−20m/s)
Δp=(175kg)(−20m/s)
Δp=−3500kg⋅m/s
The change in momentum of Percy and the bike is ∗3500kg\cdotm/sintheoppositedirectionofmotion∗
7.4 Step 1: Use the impulse-momentum theorem.
Given:
Change in momentum Δp=−3500kg⋅m/s (from 7.3)
Time taken Δt=8 s
Average frictional force Ffriction=?
Step 2: Calculate the average frictional force.
FnetΔt=Δp
In this case, the net force is the frictional force.
Ffriction(8s)=−3500kg⋅m/s
Ffriction=8s−3500kg\cdotm/s
Ffriction=−437.5 N
The magnitude of the average frictional force is ∗437.5N∗
7.5 Step 1: Calculate the distance travelled while stopping.
We need the acceleration first.
a=Δtv−u
a=8s0m/s−20m/s
a=8s−20m/s
a=−2.5m/s2
Now, calculate the distance s using a kinematic equation:
v2=u2+2as
(0m/s)2=(20m/s)2+2(−2.5m/s2)s
0=400−5s
5s=400
s=5400
s=80 m
Step 2: Calculate the work done by the frictional force.
Work done W=F⋅s⋅cosθ. The frictional force acts opposite to the direction of motion, so θ=180∘ and cos(180∘)=−1.
W=(437.5N)(80m)(−1)
W=−35000 J
Alternatively, using the work-energy theorem:
Wnet=ΔKE=KEf−KEi
KEi=21Mu2=21(175kg)(20m/s)2=21(175)(400)=35000 J
KEf=21Mv2=21(175kg)(0m/s)2=0 J
Wnet=0J−35000J=−35000 J
The work done by the frictional force is ∗35000J∗ (The negative sign indicates work done against motion).
2015 Free State Prelim Paper 1 Q4
4.1 The Law of Conservation of Momentum states that:
∗Thetotallinearmomentumofanisolatedsystemremainsconstantinbothmagnitudeanddirection.∗
4.2 The condition for an elastic collision is that ∗bothmomentumandkineticenergyareconserved.∗
4.3 Step 1: Identify the given values.
Mass of trolley mT=5 kg
Initial velocity of trolley uT=4 m/s (east, let's take east as positive)
Mass of brick mB=1.5 kg
Initial velocity of brick uB=0 m/s (dropped onto the trolley)
Step 2: Apply the principle of conservation of linear momentum to find the final velocity of the combined system.
mTuT+mBuB=(mT+mB)vf
(5kg)(4m/s)+(1.5kg)(0m/s)=(5kg+1.5kg)vf
20+0=(6.5)vf
20=6.5vf
vf=6.520
vf≈3.0769 m/s
Step 3: Calculate the change in momentum of the 5 kg trolley.
ΔpT=mTvf−mTuT
ΔpT=(5kg)(3.0769m/s)−(5kg)(4m/s)
ΔpT=15.3845kg\cdotm/s−20kg⋅m/s
ΔpT=−4.6155kg⋅m/s
The change in momentum of the 5 kg trolley is ∗4.62kg\cdotm/swest∗ (rounded to two decimal places).
2008 Exemplar Paper 1 Q 2
2.1 Step 1: Identify the given values and define a positive direction.
Let right be the positive direction.
Mass of car mC=1600 kg
Initial velocity of car uC=−30 m/s (to the left)
Mass of minibus mM=3000 kg
Initial velocity of minibus uM=20 m/s (to the right)
The vehicles move together after the collision, so they have a common final velocity vf.
Step 2: Apply the principle of conservation of linear momentum.
mCuC+mMuM=(mC+mM)vf
(1600kg)(−30m/s)+(3000kg)(20m/s)=(1600kg+3000kg)vf
−48000+60000=(4600)vf
12000=4600vf
vf=460012000
vf≈2.61 m/s
The velocity of the two vehicles after the collision is ∗2.61m/stotheright∗
2.2 Step 1: Calculate the total initial kinetic energy.
KEi=21mCuC2+21mMuM2
KEi=21(1600kg)(−30m/s)2+21(3000kg)(20m/s)2
KEi=21(1600)(900)+21(3000)(400)
KEi=800(900)+1500(400)
KEi=720000J+600000 J
KEi=1320000 J
Step 2: Calculate the total final kinetic energy.
KEf=21(mC+mM)vf2
KEf=21(1600kg+3000kg)(2.6087m/s)2
KEf=21(4600)(6.8053)
KEf=2300(6.8053)
KEf≈15652.19 J
Step 3: Compare initial and final kinetic energies.
Since KEi=1320000 J and KEf≈15652.19 J,
KEi=KEf
Therefore, kinetic energy is not conserved, and the collision was ∗inelastic∗