# Increasing water pressure to shower head

I have a 200 liter water tank 3 meters above a shower head. The tank and head are connected directly by a relatively small pipe. The shower head has an intake with a diameter the same size as the pipe leading from the tank. The water pressure coming from the head is too low.

I am tempted to believe increasing the size of the pipe from the tank to maybe two or three times of the intake of the shower will increase the water pressure into the shower.

I, like many people, use the thumb over the head of a hosepipe as method of how to increase pressure but after some reading up I have found you are trading reduced water flow for increased water pressure and in reality you have hindered the rate of water flow.

However this maybe the effect i require for the instant shower to work.

Do you think this will help?

• Welcome to Physics Stack Exchange. The question here is "Do you think this will help?" but it's not clear what "this" means. If "this" refers to increasing the diameter of the pipe connecting the reservoir to the shower head, please adjust the wording to make that as clear as possible. It's important to make questions clear so that you get good answers. Enjoy the site :-) Aug 24 '16 at 6:38 $$p=p_0+\rho gy$$ Where $p_0$ is the atmospheric pressure, $y$ the height difference between tank meniscus and shower head, $\rho$ the density of water ($g\approx 10$$\:\mathrm{m/s^2}). The water pressure coming from the head is too low. What the OP really means here is that the shower only delivers a trickle of water (low flow speed). So here I'll evaluate the factors that influence that flow speed. When flow starts, p is lowered by: 1. Viscous losses in the pipe: Acc. Darcy Weisbach pressure loss in a straight pipe due to flow is given by:$$\Delta p=f_D\frac{\rho}{2}\frac{v^2}{D}L$$Where f_D is a friction factor, v is flow speed (mathrm{m/s}), D pipe diameter and L pipe length. For laminar flow:$$f_D=\frac{64\mu}{\rho D v}$$Where \mu is the viscosity of the fluid. So for laminar flow:$$\Delta p=\frac{32\mu v}{D^2}L$$2. Local resistances: Valves, bends, kinks, sudden changes in diameter etc. all cause head loss h, usually modelled as:$$h_r=c\frac{v^2}{2g}$$Where c is a coefficient that depends on the type of local resistance. In the OP's stated problem the main local resistance is almost certainly the shower head itself. 3. Bernoulli's principle: Using Bernoulli's principle we can now write (for laminar flow):$$y=\frac{v^2}{2g}+\frac{32\mu v}{\rho gD^2}L+c_{shower}\frac{v^2}{2g}$$Or:$$y=(c_{shower}+1)\frac{v^2}{2g}+\frac{32\mu v}{\rho gD^2}L$$This is a simple quadratic equation in$v$and if$c_{shower}$and the other factors where known, then it could be solved quite easily. But in the absence of that information we can still say that$v$: • will increase with$y$, • will increase with$D$, • will decrease with$L$, • will decrease with$c_{shower}$. 4. Turbulent flow: In the case of turbulent flow (high$v$,$Re > 4000$),$f_D$becomes a function of$v$,$f_D=f(v)\$ and the calculation becomes more complicated. But the general conclusions above still hold.