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🏠 Home 🎯 Advanced ⏱ Practice

If you haven't mastered the Core Concepts and Energy Conservation pages first — go back. This page assumes you can do standard WEP problems in under 2 minutes. Come here only when you're ready.

Variable Force — Work Integral

Force as Function of Position: F(x)

Appeared in JEE Advanced 2015, 2018, 2021

★★★★ JEE Advanced

A particle of mass 1 kg moves under force F(x) = 3x² − 2x + 1 N. Find work done from x = 0 to x = 3 m and the final velocity if it started from rest at x = 0.

Newton's 2nd Law with variable force → Cannot use kinematics directly. Must integrate. W = ∫F dx → then use W = ΔKE.

  1. 1

    Work done by integrating F(x):

    W = ∫₀³ (3x² − 2x + 1) dx
    = [x³ − x² + x]₀³
    = (27 − 9 + 3) − 0 = 21 J
  2. 2

    Apply Work-Energy Theorem (u = 0):

    21 = ½ × 1 × v² → v = √42 ≈ 6.48 m/s
🎯 JEE Twist on This Concept

JEE Advanced sometimes gives F as a function of v: F = F(v). Then you need: m dv/dt = F(v) → m(dv/dx)(dx/dt) = F(v) → mv dv = F(v) dx → can't directly integrate. Need F(x). If F = F(t), use impulse-momentum, not work-energy.

Work Done Against Gravity (Variable g)

Near Earth's surface, g is constant. But for large heights (like rockets), g varies: g(r) = GM/r².

Work done to lift mass m from R to 2R
W = ∫_R^{2R} (GMm/r²) dr = GMm[−1/r]_R^{2R} = GMm/2R

This is NOT mgh. For large height problems: W = GMm(1/R − 1/(R+h)). For h << R: this reduces to mgh as expected. JEE Advanced may give: "Find work done to move satellite from R to 3R." Don't use mgh — integrate.

Force as Function of Velocity

When F = F(v), use work-energy in parametric form
W = ∫ F·v dt (using instantaneous power)

Drag force = bv² (quadratic drag). Work done by drag over displacement d = ∫₀ᵈ bv² dx. This requires knowing v(x), which comes from solving the ODE. JEE Advanced 2023 had this type.

Potential Energy Curves — Full Analysis

PE Function Analysis: U(x) = ax² − bx (a, b > 0)

★★★★★ JEE Advanced

For U(x) = 2x² − 4x (SI units). Find: (a) equilibrium position, (b) stability, (c) force at x = 1, (d) oscillation frequency if m = 1 kg.

  1. 1

    Equilibrium: dU/dx = 0

    4x − 4 = 0 → x = 1 m
  2. 2

    Stability: d²U/dx² at x = 1:

    d²U/dx² = 4 > 0 → Stable equilibrium
  3. 3

    Force at x = 1: F = −dU/dx = −(4x − 4) = −4(x−1)

    At x = 1: F = 0 ✓ (equilibrium confirmed)
  4. 4

    Since F = −k(x−1) where k = 4: This is SHM!

    ω = √(k/m) = √(4/1) = 2 rad/s
    f = ω/2π = 1/π Hz

Any potential energy function U(x) that has a stable minimum is a de facto SHM system for small oscillations. The effective spring constant is k_eff = d²U/dx² evaluated at the equilibrium point. This connects WEP to SHM in a fundamental way — a JEE Advanced signature connection.

Classically Forbidden Regions

For a particle with total energy E, the regions where U(x) > E are forbidden. The particle cannot reach there because KE would be negative (impossible).

Allowed region: KE ≥ 0
E − U(x) ≥ 0 → U(x) ≤ E

Turning points: where U(x) = E exactly (KE = 0, velocity = 0, particle reverses).

Bound vs Unbound Motion

  • Bound: E < U_max (particle oscillates between turning points)
  • Unbound: E > U_max everywhere (particle escapes to infinity)

This is how escape velocity is derived: The particle must have total energy ≥ 0 (U_∞ = 0) to escape Earth. ½mv_e² − GMm/R = 0 → v_e = √(2GM/R). Energy method beats kinematics every time for this.

Energy in Non-Inertial Frames

Work Done by Pseudo Force in Accelerating Frame

★★★★ JEE Advanced

A block of mass m rests on a wedge (mass M) on a horizontal surface. The wedge is given a horizontal acceleration a. Find the work done by the pseudo force on the block in the non-inertial frame of the wedge.

In a non-inertial (accelerating) frame, a pseudo force = ma acts on every object in the direction opposite to the frame's acceleration. Work done by pseudo force = W = F_pseudo · displacement_in_frame.

Pseudo force on block (frame accelerating at a to the right)
F_pseudo = ma (pointing left, i.e., opposite to acceleration)

Energy conservation IS valid in non-inertial frames if you include the work done by pseudo forces. This is the key. JEE Advanced: "A truck brakes suddenly. A block slides forward on the truck. Find KE gained by block in truck's frame." → Include pseudo force work.

Work-Energy Theorem in Non-Inertial Frame

Example: Ball in elevator

Elevator accelerates upward at a. Ball dropped inside. Find "effective g" seen by observer in elevator.

g_eff = g + a (upward acceleration)
g_eff = g − a (downward acceleration)

PE = mg_eff × h in the accelerating frame. Energy conservation uses g_eff.

Advanced Spring Systems

Two-Block Spring Collision

★★★★ JEE Adv

Block A (mass m) moving at v₀ collides with block B (mass 2m) at rest, connected to a spring (k). Find maximum compression and speeds after spring extension.

  1. 1

    At max compression: same velocity (momentum conservation)

    v_common = mv₀/(m+2m) = v₀/3
  2. 2

    Max compression x: Energy conservation

    ½mv₀² = ½(3m)(v₀/3)² + ½kx²
    x = v₀√(2m/3k)
  3. 3

    Final: spring elastic → equivalent to elastic collision

    v_A = (m−2m)v₀/(3m) = −v₀/3, v_B = 2v₀/3

A spring between two blocks = elastic collision in disguise. Final velocities match elastic collision formulas. Maximum compression = intermediate compressed state.

Spring Cut and Recombined

★★★ JEE Main+

A spring of constant k and natural length L is cut into 3 pieces: L/3, L/3, 2L/3. A block is attached to the two L/3 pieces in parallel. Find the period of oscillation.

  1. 1

    Each L/3 piece: k_part = 3k (halving length → doubling spring constant)

    k₁ = k₂ = 3k
  2. 2

    Two L/3 pieces in parallel:

    k_eff = 3k + 3k = 6k
  3. 3
    T = 2π√(m/6k)

How JEE Advanced Thinks About WEP

🎯 Pattern 1: Energy is the constraint

When you see "find maximum displacement" or "find turning point" — energy conservation gives you the constraint directly. Don't find the trajectory.

If you try to use kinematics for maximum displacement in a curved path → impossible. Energy: always works.

🎯 Pattern 2: Symmetry in elastic collisions

For equal mass elastic collision: velocities exchange. This is a symmetry argument, not a formula. JEE uses this in multi-ball collisions and Newton's cradle problems.

3 equal balls in a row: First hits second → 1 stops, 2 moves → 2 hits 3 → 2 stops, 3 moves. Result: 1 and 2 stop, 3 moves with original speed.

🎯 Pattern 3: F = −dU/dx yields SHM

Any PE function with a stable minimum can support SHM for small oscillations. Find d²U/dx² at equilibrium = effective k. Then ω = √(k_eff/m).

This unified approach solves: springs, pendulum, molecular vibrations, liquid in U-tube — all using one framework.

JEE Advanced signature question types that will appear again: (1) Multi-step spring-friction-incline (numerical), (2) PE curve with 4 options about equilibrium and forces (multi-correct), (3) Rolling motion energy with non-standard moment of inertia, (4) Two-body collision + spring compression + rebound analysis. If you can solve all 4 in under 20 minutes total, you're Advanced-ready.