Bernoulli's Equation — Question 5

Section 14-9 · Physics pages 2220–2221

Question 5 The lowest hole does not send a jet farthest A large open tank maintains its free surface at height H above a horizontal floor. A small horizontal outlet is at height z above the floor, with 0 < z < H. Use ideal Bernoulli discharge, negligible surface speed and projectile motion without air drag. The jet exits at atmospheric pressure. H z Horizontal jet from a small opening; heights are measured above the floor. (a) Derive the horizontal range R(z) before the jet reaches the floor. (b) Find the outlet height giving maximum range. Explain why two complementary heights z and H −z give the same range.
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Question 5 - Solution The lowest hole does not send a jet farthest H z (a) Derivation and calculation Bernoulli supplies the horizontal exit speed, while free fall supplies flight time: v = √ 2g(H −z), t = √ 2z/g. R(z) = vt = 2 √ z(H −z) . R →0 as z →0+ or z →H−. (b) Result and interpretation z(H −z) = H2/4 −(z −H/2)2 ≤H2/4. zoptimum = H/2 , Rmax = H . R(H −z) = 2 √ (H −z)z = R(z). Complementary heights interchange the speed head and flight height. A lower hole gives more speed but less flight time. Physical check The gravitational acceleration cancels from the ideal range because its effects on speed and fall time compensate.

Question 5

The lowest hole does not send a jet farthest

A large open tank maintains its free surface at height HH above a horizontal floor. A small horizontal outlet is at height zz above the floor, with 0<z<H0<z<H. Use ideal Bernoulli discharge, negligible surface speed and projectile motion without air drag. The jet exits at atmospheric pressure.

Diagram shown in the original SVG worksheet.

  1. Derive the horizontal range R(z)R(z) before the jet reaches the floor.

  2. Find the outlet height giving maximum range. Explain why two complementary heights zz and H−zH-z give the same range.

Question 5 - Solution

The lowest hole does not send a jet farthest

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Bernoulli supplies the horizontal exit speed, while free fall supplies flight time:v=2g(H−z),t=2z/g.v=\sqrt{2g(H-z)},\qquad t=\sqrt{2z/g}.R(z)=vt=2z(H−z).\boxed{R(z)=vt=2\sqrt{z(H-z)}}.R→0as z→0+ or z→H−.R\to0\quad\text{as }z\to0^+\text{ or }z\to H^-.

(b) Result and interpretation

z(H−z)=H2/4−(z−H/2)2≤H2/4.z(H-z)=H^2/4-(z-H/2)^2\le H^2/4.zoptimum=H/2,Rmax=H.\boxed{z_{\mathrm{optimum}}=H/2},\qquad\boxed{R_{\max}=H}.R(H−z)=2(H−z)z=R(z).R(H-z)=2\sqrt{(H-z)z}=R(z).Complementary heights interchange the speed head and flight height. A lower hole gives more speed but less flight time.

Physical check

The gravitational acceleration cancels from the ideal range because its effects on speed and fall time compensate.