Motion and Motion Graphs: Question 7

Syllabus 1.2

Structured Core 10 marks

A hot air balloon pilot practises controlling the balloon's height during a short test flight over flat ground. The balloon's height above the ground is recorded throughout the flight:

  • From t=0t = 0 to t=40 st = 40\text{ s}: the height increases steadily (a straight line on the graph) from 0 m0\text{ m} to 300 m300\text{ m}.
  • From t=40 st = 40\text{ s} to t=100 st = 100\text{ s}: the height continues to increase steadily (a straight line, but with a shallower gradient) from 300 m300\text{ m} to 480 m480\text{ m}.
  • From t=100 st = 100\text{ s} to t=160 st = 160\text{ s}: the pilot begins a controlled descent. The height decreases from 480 m480\text{ m} to 120 m120\text{ m}, but this section of the graph is a curve, not a straight line: it is steep immediately after t=100 st = 100\text{ s} and becomes less steep as tt approaches 160 s160\text{ s}.

(a) Calculate the balloon's ascent speed during the first section, from t=0t = 0 to t=40 st = 40\text{ s}. [2]

(b) Calculate the balloon's ascent speed during the second section, from t=40 st = 40\text{ s} to t=100 st = 100\text{ s}. State which of the two ascent sections has the greater speed, and explain how this is shown by the steepness of the two lines. [2]

(c) State whether the balloon's descent speed during the third section is constant, increasing, or decreasing, and explain how you can tell this from the shape of the graph. [2]

(d) Calculate the balloon's average descent speed for the whole third section, from t=100 st = 100\text{ s} to t=160 st = 160\text{ s}. Explain why this value is not equal to the balloon's actual descent speed at every instant during this section. [3]

(e) Calculate the total distance travelled by the balloon (vertically) during the whole 160 s160\text{ s} flight described above. [1]

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Worked solution

Part (a): Ascent speed during the first section

Speed is the gradient of a distance–time (here, height–time) graph, v=ΔsΔtv = \dfrac{\Delta s}{\Delta t}. During the first section, the height increases from 0 m0\text{ m} to 300 m300\text{ m} over 40 s40\text{ s}:

v1=300 m40 s=7.5 m/sv_1 = \frac{300\text{ m}}{40\text{ s}} = 7.5\text{ m/s}

Part (b): Ascent speed during the second section

During the second section, the height increases from 300 m300\text{ m} to 480 m480\text{ m}:

Δs=480 m300 m=180 m,Δt=100 s40 s=60 s\Delta s = 480\text{ m} - 300\text{ m} = 180\text{ m}, \qquad \Delta t = 100\text{ s} - 40\text{ s} = 60\text{ s}

v2=180 m60 s=3.0 m/sv_2 = \frac{180\text{ m}}{60\text{ s}} = 3.0\text{ m/s}

Comparing the two sections, 7.5 m/s>3.0 m/s7.5\text{ m/s} > 3.0\text{ m/s}, so the first section has the greater ascent speed. This is shown on the graph by the first section’s line being steeper than the second section’s line. A larger gradient means a greater speed, even though the balloon is still rising (not falling) in both sections.

Part (c): Interpreting the curved third section

The third section is a curve, not a straight line, so its gradient is not constant. The curve is steep immediately after t=100 st = 100\text{ s} and becomes less steep as tt approaches 160 s160\text{ s}. Since the (downward) gradient of a height-time graph gives the descent speed, a gradient that is shrinking in magnitude means the balloon’s descent speed is decreasing throughout this section, it descends quickly at first and gradually slows down as it approaches the end of the section.

Part (d): Average descent speed over the third section

The area under a curve cannot be used to find a single speed here. Instead, the average speed over the whole section uses the total change in height and the total time taken, ignoring how the speed varies within that interval:

Δs=480 m120 m=360 m,Δt=160 s100 s=60 s\Delta s = 480\text{ m} - 120\text{ m} = 360\text{ m}, \qquad \Delta t = 160\text{ s} - 100\text{ s} = 60\text{ s}

vavg=360 m60 s=6.0 m/sv_{\text{avg}} = \frac{360\text{ m}}{60\text{ s}} = 6.0\text{ m/s}

This value of 6.0 m/s6.0\text{ m/s} is not the balloon’s actual descent speed at every instant. Because this section of the graph is a curve rather than a straight line, the descent speed is continuously changing (decreasing, as found in part (c)): it is greater than 6.0 m/s6.0\text{ m/s} just after t=100 st = 100\text{ s} and less than 6.0 m/s6.0\text{ m/s} as tt approaches 160 s160\text{ s}. This is unlike the first and second sections, where the straight lines mean the calculated speed is the actual, constant speed for the whole section.

Part (e): Total distance travelled during the flight

The total distance travelled adds the size of the height change in every section, regardless of whether the balloon was rising or falling:

total distance=300 m+180 m+360 m\text{total distance} = 300\text{ m} + 180\text{ m} + 360\text{ m}

total distance=840 m\text{total distance} = 840\text{ m}

Final answers

  • (a) Ascent speed in the first section == 7.5 m/s7.5\text{ m/s}
  • (b) Ascent speed in the second section == 3.0 m/s3.0\text{ m/s}; the first section is faster, shown by its steeper line
  • (c) The descent speed in the third section is decreasing, shown by the curve becoming less steep
  • (d) Average descent speed over the third section == 6.0 m/s6.0\text{ m/s}, which is only an average since the actual speed keeps changing
  • (e) Total distance travelled during the whole flight == 840 m840\text{ m}