Work, Energy and Power: Question 3

Syllabus 5.1, 5.2

Structured AS 8 marks

An electric winch is used to lift a steel beam of mass 250 kg250\text{ kg} vertically upward at a constant speed. The beam rises through a height of 8.0 m8.0\text{ m} in a time of 20 s20\text{ s}.

Take g=9.81 m s2g = 9.81\text{ m s}^{-2}.

(a) Show that the increase in gravitational potential energy of the beam is about 1.96×104 J1.96\times10^{4}\text{ J}. [2]

(b) Calculate the useful output power of the winch motor as it lifts the beam. [2]

(c) The winch motor has an efficiency of 75%75\%. Calculate the total power input to the motor. [2]

(d) Calculate the total energy supplied to the motor during the 20 s20\text{ s} lift. [2]

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Worked solution

Part (a): Showing the increase in gravitational PE

The beam rises at constant speed, so all the useful work done goes into increasing its gravitational PE: ΔEp=mgΔh=250×9.81×8.0\Delta E_p = mg\Delta h = 250\times9.81\times8.0

Working in two steps: 250×9.81=2452.5250\times9.81=2452.5, then 2452.5×8.0=19620 J2452.5\times8.0=19620\text{ J}.

Check by recomputing the second step differently: 2452.5×8.0=2452.5×8=19620 J2452.5\times8.0=2452.5\times8=19620\text{ J} (since 2452.5×4=98102452.5\times4=9810 and 9810×2=196209810\times2=19620). Both routes agree.

So ΔEp=19620 J=1.962×104 J\Delta E_p = 19620\text{ J} = 1.962\times10^{4}\text{ J}, which rounds to 1.96×104 J\boxed{1.96\times10^{4}}\text{ J} (3 s.f.), as required to show.

Part (b): Useful output power

Power is the rate of doing (useful) work, P=WtP=\dfrac{W}{t}. The useful work done by the motor equals the gain in gravitational PE found in part (a): Puseful=ΔEpt=1962020=981 WP_{\text{useful}} = \frac{\Delta E_p}{t} = \frac{19620}{20} = 981\text{ W}

Check: 981×20=19620 J981\times20=19620\text{ J}, which matches ΔEp\Delta E_p from part (a). Confirmed.

Part (c): Total power input

Efficiency is the ratio of useful power output to total power input: efficiency=PusefulPinput\text{efficiency} = \frac{P_{\text{useful}}}{P_{\text{input}}}

Rearranging for the total input power, using efficiency =0.75=0.75 (not 7575): Pinput=Pusefulefficiency=9810.75=1308 WP_{\text{input}} = \frac{P_{\text{useful}}}{\text{efficiency}} = \frac{981}{0.75} = 1308\text{ W}

Check: 1308×0.75=981 W1308\times0.75 = 981\text{ W}, matching PusefulP_{\text{useful}} from part (b). Confirmed. Note that Pinput>PusefulP_{\text{input}}>P_{\text{useful}}, as expected for any real, non-ideal motor.

Part (d): Total energy supplied

The total input energy is the total input power multiplied by the time for which it acts: Einput=Pinput×t=1308×20=26160 JE_{\text{input}} = P_{\text{input}}\times t = 1308\times20 = 26160\text{ J}

Check using an independent route: the total input energy must also equal the useful energy output divided by the efficiency, Einput=ΔEp/efficiency=19620/0.75=26160 JE_{\text{input}}=\Delta E_p/\text{efficiency}=19620/0.75=26160\text{ J}. Both routes agree exactly, confirming the answer.

So Einput=26160 J2.62×104 JE_{\text{input}} = \boxed{26160}\text{ J} \approx 2.62\times10^{4}\text{ J} (3 s.f.).

Final answers

  • (a) ΔEp=19620 J1.96×104 J\Delta E_p = \boxed{19620}\text{ J} \approx 1.96\times10^{4}\text{ J} (shown)
  • (b) Useful output power =981 W= \boxed{981}\text{ W}
  • (c) Total input power =1308 W= \boxed{1308}\text{ W}
  • (d) Total input energy =26160 J2.62×104 J= \boxed{26160}\text{ J} \approx 2.62\times10^{4}\text{ J}