Q.A block of mass m=1 kg, moving on a horizontal surface with speed vi=2 m s−1 enters a rough patch ranging from x=0.10 m to x=2.01 m. The retarding force Fr on the block in this range is inversely proportional to x over this range,
[!FORMULA]
Fr=−xkfor 0.1<x<2.01 m
[!FORMULA]
=0for x<0.1 m and x>2.01 m
where k=0.5 J. What is the final kinetic energy and speed vf of the block as it crosses this patch?
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The Work-Energy Theorem: From Intuition to Precision
Imagine pushing a heavy box across the floor. The harder you push and the farther it slides, the faster it moves when you let go. That connection — the push (force) over a distance (displacement) changing the box's speed — is exactly what the Work-Energy Theorem captures.
The Intuition First
Think of work as the "currency" that buys motion. When you do work on an object, you transfer energy to it. That energy shows up as kinetic energy — the energy of motion. The more work you do, the more the object's kinetic energy changes.
If you push a stationary ball, it starts moving. If you push a moving ball in the same direction, it speeds up. If you push against its motion, it slows down. In every case, the work done equals the change in the ball's kinetic energy.
Work is done by a force on an object. The object's kinetic energy changes by exactly that amount (assuming no other forces do work).
The Precise Statement
Wnet=ΔK=Kf−Ki
Where:
- Wnet is the net work done on the object (the total work from all forces combined)
- Kf is the final kinetic energy
- Ki is the initial kinetic energy
And kinetic energy is defined as:
K=21mv2
So the theorem can also be written as:
Wnet=21mvf2−21mvi2
Why "Net" Work Matters
This is the most common point of confusion. The theorem uses net work — the work done by the net force (the vector sum of all forces). If you push a box and friction opposes it, the net work is the work you do minus the work friction does. Only that net amount changes the kinetic energy.
If you push a box at constant speed, your work is positive, but friction does equal negative work. The net work is zero, so kinetic energy doesn't change — the box keeps moving at the same speed. Your work didn't "disappear"; it was dissipated as heat by friction.
A Simple Derivation (for constant force)
Consider a constant net force Fnet acting on an object of mass m over a displacement s. From Newton's second law:
Fnet=ma
From kinematics (constant acceleration):
vf2=vi2+2as
Multiply both sides by 21m:
21mvf2=21mvi2+mas
But mas=Fnets=Wnet, so:
21mvf2=21mvi2+Wnet
Rearranging:
Wnet=21mvf2−21mvi2=ΔK
The theorem holds even for variable forces and curved paths — the derivation uses calculus then, but the result is the same.
What It Tells You (and What It Doesn't) …
Concept: Work–Energy Theorem — the net work done by all forces equals the change in kinetic energy.
Step 1 – Work done by the retarding force
Only the rough patch does work. The force is Fr=−k/x, so the work is
W=∫xixfFrdx=∫0.102.01−xkdx=−k[lnx]0.102.01.
Step 2 – Evaluate the integral
W=−0.5(ln2.01−ln0.10)=−0.5ln(0.102.01)=−0.5ln(20.1).
Since ln(20.1)≈3.00,
W≈−0.5×3.00=−1.50 J.
Step 3 – Apply Work–Energy Theorem …
Because the retarding force varies with position, its work is found by integration: W=−kln(20.1)≈−1.5 J. The work-energy theorem then gives Kf=0.50 J and vf=1.0 m s−1.
The force depends on position, so work cannot be "force x distance"; it must be integrated. The work-energy theorem then converts that work directly into the change in kinetic energy.
Work done by the retarding force
W=∫0.102.01Frdx=∫0.102.01(−xk)dx=−k[lnx]0.102.01=−kln(0.102.01)=−kln(20.1).
With k=0.5 J and ln(20.1)≈3.00,
W≈−0.5×3.00=−1.5 J.
Initial kinetic energy …
Concept: Work-Energy Theorem with a Position-Dependent Force (Integration)
Step 1: Set up the work integral for the variable retarding force.
W=∫0.102.01Frdx=∫0.102.01(−xk)dx=−k[lnx]0.102.01=−kln(0.102.01)
Step 2: Evaluate numerically with k=0.5J.
W=−0.5ln(20.1)≈−0.5×3.00=−1.50J
Step 3: Apply the work-energy theorem. …
- KCET 2025Set D-41 markMCQQ.A potential at a point A is −3 V and that at another point B is 5 V. What is the work done in carrying a charge of 5mC from B to A? (A) −0.04 J (B) −0.4 J (C) −4 J (D) −40 J
›Reveal solutionSolution
Use W=qΔV=q(Vfinal−Vinitial)=q(VA−VB), being careful to convert millicoulombs to coulombs and to subtract the potentials in the right order (B → A).
Step 1 — The concept: potential difference is work per unit charge
The potential difference between two points is defined as the work done by an external agent in carrying a unit positive charge from one to the other, slowly (without changing its kinetic energy):
VA−VB=qWB→A
Rearranged, this gives the working formula:
WB→A=q(VA−VB)
Equivalently, W equals the change in electrostatic potential energy, W=ΔU=UA−UB=qVA−qVB. Since electrostatic force is conservative, this depends only on the endpoints — the path taken is irrelevant.
Step 2 — Identify the initial and final points (order matters!)
The charge is carried from B to A. So:
- Initial point = B, with VB=+5 V
- Final point = A, with VA=−3 V
The potential difference we need is Vfinal−Vinitial=VA−VB — not the other way round. Reversing this is the single most common error here and simply flips the sign.
VA−VB=(−3)−(+5)=−8 V
Step 3 — Convert the charge to SI units
q=5 mC=5×10−3 C
(The prefix milli = 10−3. Forgetting this conversion gives −40 J — option (D), a deliberate trap. Mistaking mC for μC would give −4×10−5 J.)
Step 4 — Substitute
W=q(VA−VB)=(5×10−3 C)×(−8 V)
W=−40×10−3 J=−0.04 J
W=−0.04 J
Step 5 — Why is the sign negative? (Check the physics)
The negative sign is not an accident — it carries real meaning. …
- COMEDK 2025Set 2025-E1 markMCQQ.A particle of mass 3 g and charge 60μC is released from rest in a uniform electric field of intensity 105NC−1. If the value of kinetic energy attained by the particle after moving through a distance of 2 cm is m×10−2J, then the value of m is: (A) 12 (B) 6 (C) 5 (D) 4
›Reveal solutionSolution
The kinetic energy gained equals the work done by the electric field: qEd. Substituting the given values yields 1.2×10−1J, so m=12. The correct option is (A).
Concept & Intuition
When a charged particle is released from rest in a uniform electric field, the field exerts a constant force F=qE on it. This force does work as the particle moves, and that work is entirely converted into kinetic energy (since no other forces act). The work done by a constant force over a displacement d is simply Fd. So the kinetic energy after moving distance d is K=qEd. No need to involve mass or acceleration — the energy approach is direct.
Step-by-step solution
-
Identify the given quantities
- Mass m=3g=3×10−3kg (not needed for energy, but given)
- Charge q=60μC=60×10−6C=6×10−5C
- Electric field E=105N/C
- Distance moved d=2cm=2×10−2m
-
Work done by the electric field
The force on the particle is F=qE. Since the field is uniform, the force is constant. The work done over displacement d is:
W=Fd=qEd
Substitute the values:
W=(6×10−5)×(105)×(2×10−2)
- Simplify step by step First, 6×10−5×105=6×100=6. Then multiply by 2×10−2:
-
- COMEDK 2025Set 2025-M1 markMCQQ.A vertical spring of spring constant 24Nm−1 is fixed on a table. A ball of mass 0.5 kg at a height 2 m above the free upper end of the spring falls vertically on the spring so that the spring is compressed by a distance of 50 cm . The net work done in the process is: (A) 6.5 J (B) 10.5 J (C) 12.5 J (D) 9.5 J
›Reveal solutionSolution
Total fall =2+0.5=2.5m, so gravity does mgh=12.5J while 21kx2=3J is stored in the spring; the net work done in the process is 12.5−3=9.5J — option (D).
Concept. As the ball drops onto the spring and compresses it, gravity does positive work over the whole fall, and part of that energy is stored as elastic potential energy in the spring. The net work done in the process is the work delivered by gravity minus the energy locked up in the spring.
Step 1 — Total vertical drop.
The ball starts 2m above the free (upper) end of the spring and the spring is compressed by 50cm=0.5m, so the ball descends
h=2+0.5=2.5 m.
Step 2 — Work done by gravity.
With m=0.5kg and g=10m s−2,
Wgrav=mgh=0.5×10×2.5=12.5 J. …
- COMEDK 2024Set 2024-E1 markMCQQ.A scooter moves with a speed of 7 ms−1, on a straight road and is stopped by applying the brakes. Before stopping, the scooter travels 10 m. If the weight of the scooter is W, then the total resistance to the motion of the scooter will be (A) 21W (B) 41W (C) 4W (D) 2W
›Reveal solutionSolution
Using the work–energy theorem, the braking force does work equal to the loss in kinetic energy. The computed resistance is one‑quarter of the scooter’s weight, so the correct option is (B).
The key idea is that the brakes apply a constant resisting force (the total resistance to motion) over the stopping distance. The work done by that force equals the change in kinetic energy. Because the weight W is given, we can express the mass as m=W/g and then solve for the force in terms of W.
-
Identify the known quantities
Initial speed: u=7 m/s
Stopping distance: s=10 m
Final speed: v=0
Weight of scooter: W (in newtons)
Acceleration due to gravity: g=9.8 m/s2 (we will keep it symbolic initially).
-
Relate force to acceleration using kinematics
From v2=u2+2as, we get
0=(7)2+2a(10)⇒49+20a=0⇒a=−2049=−2.45 m/s2.
The negative sign means deceleration. The magnitude of the acceleration is a=2.45 m/s2.
- Apply Newton’s second law The total resisting force F (assumed constant) is
F=ma,
where m is the mass. Since weight W=mg, we have m=W/g. Thus
F=gW⋅a.
- Substitute numbers Using g=9.8 m/s2 and a=2.45 m/s2:
-
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