HC Verma Chapter 3 Problem 19 — Velocity components of horizontal projectile at t

Problem Statement

Solve the kinematics problem: A ball is thrown horizontally at 10 m/s. Find its speed after 3 s. ($g = 10$ m/s²) $v_x = 10$ m/s (constant); $v_y = gt$ (downward) $v = \sqrt{v_x^2 + v_y^2}$ Step 1: $v_y = 10 \times 3 = 30$ m/s. Step 2: $v = \sqrt{100 + 900} = \sqrt{1000} = 10\sqrt{10} \approx 31.6$ m/s. $$\boxed{v = 10\sqrt{10} \

Given Information

  • See problem statement for all given quantities.

Physical Concepts & Formulas

Projectile motion decomposes into independent horizontal and vertical components. Horizontal: constant velocity (no air resistance). Vertical: constant downward acceleration $g$. The trajectory is a parabola. Maximum range occurs at $45°$ launch angle; max height at $90°$.

  • $x = v_0\cos\theta \cdot t$, $y = v_0\sin\theta \cdot t – \frac{1}{2}gt^2$
  • $R = v_0^2\sin 2\theta/g$ — horizontal range
  • $H = v_0^2\sin^2\theta/(2g)$ — maximum height
  • $T = 2v_0\sin\theta/g$ — total flight time

Step-by-Step Solution

Step 1 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Step 2 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Step 3 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Worked Calculation

$$\boxed{v = 10\sqrt{10} \

Given Information

  • Initial velocity $u$ (or $v_0$)
  • Acceleration $a$ (constant unless stated otherwise)
  • Time $t$ or distance $s$ as given

Physical Concepts & Formulas

Kinematics describes motion without reference to its cause. For constant acceleration, the four SUVAT equations are sufficient to solve any problem. They follow directly from the definitions of velocity ($v = ds/dt$) and acceleration ($a = dv/dt$). For 2D problems (projectile motion), the horizontal and vertical motions are independent — horizontal: constant velocity; vertical: constant acceleration $g$ downward. Relative motion problems require defining a reference frame explicitly and using vector subtraction.

  • $v = u + at$
  • $s = ut + \tfrac{1}{2}at^2$
  • $v^2 = u^2 + 2as$
  • $s = \tfrac{1}{2}(u+v)t$
  • Range of projectile: $R = \dfrac{u^2\sin 2\theta}{g}$
  • Max height: $H = \dfrac{u^2\sin^2\theta}{2g}$

Step-by-Step Solution

Step 1 — List knowns and unknown: $u$, $v$, $a$, $s$, $t$ — identify which three are known.

Step 2 — Choose the SUVAT equation that contains the unknown and all three known quantities.

Step 3 — Substitute and solve algebraically.

Step 4 — For 2D: Decompose $\vec{u}$ into $u_x = u\cos\theta$, $u_y = u\sin\theta$. Solve $x$ and $y$ separately.

Worked Calculation

Substituting all values with units:

Projectile at $u = 20\,\text{m/s}$, $\theta = 30°$:

$$

$$

$$

$$

Answer

$$

Answer

$$\boxed{R = \dfrac{u^2\sin 2\theta}{g},\quad H = \dfrac{u^2\sin^2\theta}{2g}}$$

Physical Interpretation

The trajectory is a parabola because gravity provides constant downward acceleration while horizontal velocity remains constant (absent air resistance). Real projectiles deviate due to drag, especially at high speeds.


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