---
title: "Wheel pulled by cord on inner drum, 50 kg"
subject: "Applied Mechanics (Dynamics)"
chapter: 5
key: "semester_3/applied_mechanics_dynamics:wheel-inner-drum-50kg"
source: https://www.bctengineer.com/q/semester_3/applied_mechanics_dynamics/wheel-inner-drum-50kg
site: BCT Engineering
---

# Wheel pulled by cord on inner drum, 50 kg

Applied Mechanics (Dynamics) · Chapter 5: Plane Motion of Rigid Bodies: Forces, Moments, and Accelerations

- Asked in: 2080 Bhadra, 6 marks
- Video: [A cord is wrapped around the inner drum of a wheel and pull horizontally with force 200N](https://www.youtube.com/watch?v=uVJ7zkIVLPU) — Civil Engg Network
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_3/applied_mechanics_dynamics/wheel-inner-drum-50kg
- Whole chapter: https://www.bctengineer.com/md/semester_3/applied_mechanics_dynamics/chapter-5

## Question

A cord wrapped around the inner drum of a wheel and pulled horizontally with a force of 200 N. The wheel has a mass of 50 kg and a radius of gyration of 70 mm. Knowing that the coefficients of friction are $\mu_s = 0.20$ and $\mu_k = 0.15$, determine the acceleration of G and the angular acceleration of the wheel. [Figure: wheel with outer radius 100 mm and inner drum radius 60 mm; 200 N pulled horizontally to the right by the cord on the inner drum; wheel on rough ground.]

## Short answer

Rolling assumption fails because required friction exceeds μ_s N. With kinetic friction 73.58 N, a_G = (200−73.58)/50 = 2.53 m/s² right. I = mk² = 0.245 kg·m²; α = (200×0.06−73.58×0.10)/0.245 = 18.95 rad/s² CCW.

## Answer

**Assumptions.** The cord leaves the bottom of the inner drum (radius $r=0.060$ m) and pulls horizontally to the right; the wheel (outer radius $R=0.100$ m) rests on rough ground. Take $x$ to the right; the sense of $\alpha$ is stated in each step. The friction force $F$ acts at the contact point.

#### Data
$m = 50$ kg, $\bar k = 0.070$ m, $P = 200$ N, $\mu_s = 0.20$, $\mu_k = 0.15$

$$
\bar I = m\bar k^2 = 50(0.070)^2 = 0.2450\ \text{kg m}^2, \qquad N = mg = 50\times9.81 = 490.50\ \text{N}
$$

#### Step 1: assume rolling without slipping
Rolling to the right means the wheel turns clockwise, so $\bar a = \alpha R$ with $\alpha$ clockwise. The pull $P$ (below $G$) gives a counter-clockwise moment $Pr$ about $G$; friction $F$, taken to the left at the contact point, gives a clockwise moment $FR$:

$$
\begin{aligned}
P - F &= m\bar a\\
FR - Pr &= \bar I\alpha
\end{aligned}
$$

Eliminating $F$ with $\bar a=\alpha R$:

$$
\alpha = \frac{P(R-r)}{m(\bar k^2 + R^2)} = \frac{200(0.100-0.060)}{50(0.0049+0.0100)} = 10.74\ \text{rad/s}^2\ \text{(clockwise)}, \qquad \bar a = \alpha R = 1.07\ \text{m/s}^2
$$

Friction required: $F = P - m\bar a = 200 - 50(1.07) = 146.31$ N.

Maximum available: $F_{max} = \mu_s N = 0.20\times490.50 = 98.10$ N.

Since $F = 146.31\ \text{N} > F_{max}$, the wheel **slips**. The assumption is wrong, and kinetic friction acts: $F = \mu_k N = 0.15\times490.50 = 73.58$ N.

#### Step 2: sliding (kinetic friction)
$$
\begin{aligned}
\bar a &= \frac{P - F_k}{m} = \frac{200 - 73.58}{50} = 2.53\ \text{m/s}^2\ (\to)\\
\alpha &= \frac{Pr - F_kR}{\bar I} = \frac{200(0.060) - 73.58(0.100)}{0.2450} = 18.95\ \text{rad/s}^2\ \text{(counter-clockwise)}
\end{aligned}
$$

With $\alpha$ counter-clockwise, the contact point accelerates forward relative to the ground ($\bar a + \alpha R>0$), so it slips forward. This confirms that friction acts to the left.

**Answer: $\bar a_G = 2.53$ m/s² to the right; $\alpha = 18.95$ rad/s² counter-clockwise.**

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What is the first step in solving this friction problem?
   A. Assume kinetic friction at once
   B. Assume rolling without slipping, a = alpha R, and compute the required friction
   C. Ignore friction
   D. Assume F = mu_s N
   Answer: B. Assume rolling, find the friction needed, then compare with the maximum available. (Key point: Rolling assumption)

2. Required friction is 146.31 N while mu_s N = 98.1 N. What follows?
   A. The wheel rolls without slipping
   B. The wheel slips, so kinetic friction F = mu_k N acts
   C. The wheel lifts off
   D. Friction is zero
   Answer: B. Required friction exceeds the static maximum, so the wheel slips and F = mu_k N = 73.58 N. (Key point: Slip check)

3. With F_k = 73.58 N, P = 200 N, m = 50 kg, a_G is:
   A. 2.53 m/s^2
   B. 1.07 m/s^2
   C. 4.0 m/s^2
   D. 5.47 m/s^2
   Answer: A. a = (200 - 73.58)/50 = 2.53 m/s^2 to the right. (Key point: Acceleration of G)

4. Which expression gives alpha when sliding?
   A. (P R - F r)/I
   B. (P r - F_k R)/I
   C. P r / I
   D. (P - F_k) / I
   Answer: B. Moments about G: P r - F_k R = I alpha, giving 18.95 rad/s^2 counter-clockwise. (Key point: Angular acceleration)

## Close variants set in other exams

- [Wheel pulled by cord on inner drum, 45 kg](https://www.bctengineer.com/question.md?key=semester_3%2Fapplied_mechanics_dynamics%3Awheel-inner-drum-45kg) — Applied Mechanics (Dynamics), chapter 5, asked 2×

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