9709/41

Mathematics 9709/41October/November 2014

Cambridge AS Level · Mechanics · worked solutions for every part, with the mark scheme

7
questions
50
marks
75
minutes

Topics Newton's Laws of Motion · Forces and Equilibrium · Energy, Work and Power · Kinematics of Motion in a Straight Line

Q14MEnergy, Work and PowerNewton's Laws of MotionFree sample

A car of mass 800 kg800\text{ kg} is moving on a straight horizontal road with its engine working at a rate of 22.5 kW22.5\text{ kW}. Find the resistance to the car's motion at an instant when the car's speed is 18 m s118\text{ m s}^{-1} and its acceleration is 1.2 m s21.2\text{ m s}^{-2}.

DifficultyMedium-Easy
Worked solution

Approach

Use the power–velocity relation P=FvP = Fv to find the driving force DFDF, then apply Newton's second law along the horizontal direction. The engine force acts forwards and the resistance acts backwards, so DFR=maDF - R = ma.

Working

Engine power:

P=22.5 kW=22500 WP = 22.5\text{ kW} = 22500\text{ W}

Driving force from P=DF×vP = DF \times v:

DF=Pv=2250018=1250 NDF = \frac{P}{v} = \frac{22500}{18} = 1250\text{ N}

Newton's second law horizontally:

DFR=maDF - R = ma 1250R=800×1.2=9601250 - R = 800 \times 1.2 = 960

Solve for RR:

R=1250960=290 NR = 1250 - 960 = 290\text{ N}

Answer

The resistance to the car's motion is 290 N290\text{ N}.

Final answer

290 N

Detailed explanation

Walkthrough

The car is moving on a horizontal road, so we only need to consider horizontal forces: the driving force DFDF from the engine and the resistance RR opposing the motion. The engine power is 22.5 kW22.5\text{ kW}, which is 22500 W22500\text{ W} because 1 kW=1000 W1\text{ kW} = 1000\text{ W}.

For a constant power output, P=FvP = Fv, so the driving force at this instant is

DF=Pv=2250018=1250 N.DF = \frac{P}{v} = \frac{22500}{18} = 1250\text{ N}.

Now apply Newton's second law in the direction of motion. The resultant horizontal force is DFRDF - R, since RR opposes the motion, and this must equal mama:

DFR=800×1.2=960.DF - R = 800 \times 1.2 = 960.

Substitute DF=1250DF = 1250:

1250R=960,1250 - R = 960,

so

R=1250960=290 N.R = 1250 - 960 = 290\text{ N}.

The resistance is therefore 290 N290\text{ N}.

Key Takeaways

  • Power and force are related by P=FvP = Fv at the instant considered.
  • In horizontal motion with forward and backward forces, Newton's second law requires the resultant force: Fresultant=maF_{\text{resultant}} = ma.
  • Resistance is a force that acts opposite to the direction of motion, so it is subtracted from the driving force.
  • Units must be consistent: kilowatts must be converted to watts before using P=FvP = Fv.

Common Mistakes

  • Forgetting to convert 22.5 kW22.5\text{ kW} to 22500 W22500\text{ W}, which would give a wrong driving force.
  • Writing Newton's second law as DF+R=maDF + R = ma instead of DFR=maDF - R = ma. Since RR opposes the motion, it must be subtracted.
  • Quoting the resistance without showing the Newton's second law equation; the mark scheme awards a method mark for using three terms, so working must be shown.
  • Using DF=P×vDF = P \times v instead of DF=P/vDF = P/v.

Things to Be Careful About

  • The driving force is instantaneous because the power and speed are given at that instant.
  • Check the direction: the engine force is in the direction of motion, while the resistance opposes it.
  • The final answer must be in newtons.
  • If the acceleration were negative, the sign of mama would change, but here acceleration is positive in the direction of motion.
Techniques used
convert engine power to driving force using P = Fvapply Newton's second law to horizontal motionsolve for the resistance force

The rest of this paper

6 more questions
  • Q2Newton's Laws of Motion · Forces and Equilibrium4M
  • Q3Forces and Equilibrium6M
  • Q4Kinematics of Motion in a Straight Line7M
  • Q5Forces and Equilibrium · Newton's Laws of Motion9M
  • Q6Newton's Laws of Motion · Kinematics of Motion in a Straight Line9M
  • Q7Energy, Work and Power11M
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