Work Done on a System by an External Force — Question 2

Section 8-6 · Physics pages 1114–1115

Question 2 Pulling across a rough surface inside the system Assume no heat transfer across the stated system boundary during the process unless otherwise specified. A 2 kg block starts from rest and is pulled horizontally 5 m by a constant 12 N force. Sliding friction is 4 N. Choose block plus floor as the system, and neglect floor recoil. block 12 N The dashed boundary encloses both surfaces; the pulling agent remains outside. (a) Find external pulling work and the increase in thermal energy. (b) Find final block speed. (c) Explain why subtracting friction work and also adding the same thermal rise on the energy-output side would double-count dissipation.
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Question 2 - Solution Pulling across a rough surface inside the system block 12 N (a) Separate input from internal conversion. The pulling agent supplies energy while rubbing converts part into an internal thermal store: Wpull = 12(5) = 60 J , ∆Eth = 4(5) = 20 J . (b) Use the full energy balance. For block plus floor, 60 = Kf + 20 ⇒Kf = 40 J, vf = √ 2(40)/2 = √ 40 = 6.325 m/s . (c) Choose a consistent form. The equivalent balances use different boundaries: block motion: Wpull −fkd = ∆K, block + floor: Wpull = ∆K + ∆Eth. Using both −fkd and the same thermal term in the larger-system balance would count the 20 J conversion twice.

Question 2

Pulling across a rough surface inside the system

Assume no heat transfer across the stated system boundary during the process unless otherwise specified. A 2 kg block starts from rest and is pulled horizontally 5 m by a constant 12 N force. Sliding friction is 4 N. Choose block plus floor as the system, and neglect floor recoil.

Diagram shown in the original SVG worksheet.

  1. Find external pulling work and the increase in thermal energy.

  2. Find final block speed.

  3. Explain why subtracting friction work and also adding the same thermal rise on the energy-output side would double-count dissipation.

Question 2 - Solution

Pulling across a rough surface inside the system

Diagram shown in the original SVG worksheet.

(a) Separate input from internal conversion.

The pulling agent supplies energy while rubbing converts part into an internal thermal store: Wpull=12(5)=60J,ΔEth=4(5)=20J.\boxed{W_{\mathrm{pull}}=12(5)=60\ \mathrm J},\qquad\boxed{\Delta E_{\mathrm{th}}=4(5)=20\ \mathrm J}.

(b) Use the full energy balance.

For block plus floor, 60=Kf+20⇒Kf=40J,60=K_f+20\Rightarrow K_f=40\ \mathrm J, vf=2(40)/2=40=6.325m/s.\boxed{v_f=\sqrt{2(40)/2}=\sqrt{40}=6.325\ \mathrm{m/s}}.

(c) Choose a consistent form.

The equivalent balances use different boundaries: block motion: Wpull−fkd=ΔK,\text{block motion: }W_{\mathrm{pull}}-f_kd=\Delta K, block + floor: Wpull=ΔK+ΔEth.\text{block + floor: }W_{\mathrm{pull}}=\Delta K+\Delta E_{\mathrm{th}}. Using both −fkd-f_kd and the same thermal term in the larger-system balance would count the 20 J conversion twice.