Skip to content
Exercise · Q11

Q.What physical quantity is represented by the area under a velocity-time graph? Justify your answer using the integral relationship between velocity and position.

West Bengal WbchseTextbookSubjectiveImportance★★★★★
46% · 11/24 Questions
🔒 Locked · start free trial →

You're viewing a preview — the full solution, concept, methods & PYQ mapping are locked.

Start your 14-day free trial to unlock the full solution →

The defining relation. Instantaneous velocity is defined as v=dx/dtv = dx/dt (Section 2.4), which rearranges to dx=v dtdx = v\,dt.

Integrating. To find the net change in position (displacement) between times t1t_1 and t2t_2, we integrate both sides:

∫x1x2dx=∫t1t2v dt⟹x2−x1=∫t1t2v dt\int_{x_1}^{x_2} dx = \int_{t_1}^{t_2} v\,dt \quad\Longrightarrow\quad x_2 - x_1 = \int_{t_1}^{t_2} v\,dt

Geometric meaning of the integral. The definite integral ∫t1t2v dt\int_{t_1}^{t_2} v\,dt is, by the fundamental geometric definition of a definite integral, exactly the signed area enclosed between the curve v(t)v(t) and the time axis, between the vertical lines t=t1t = t_1 and t=t2t = t_2 — any portion of the curve above the axis (positive vv) contributes positive area, and any portion below the axis (negative vv, i.e. motion in the negative direction) contributes negative area.

Conclusion. Combining the two results directly gives

Δx=x2−x1=area under the v-t graph between t1 and t2\Delta x = x_2 - x_1 = \text{area under the } v\text{-}t \text{ graph between } t_1 \text{ and } t_2 …

Unlock everything free for 14 days

  • Full step-by-step solutions
  • Concept-first explanations
  • Methods, shortcuts & mistakes
  • PYQ mapping + timed mock tests

Full access for 14 days. No credit card required.