clear
clc
%% Note:
% In the given problem it is mentioned P1 is 3 kPa and air is
flowing out.
% This means the mentioned pressure is gauge pressure. Because If
it is
% absolute pressure then as outside air pressure is 101.325 kPa,
flow should
% be into the system, but it is not. Hence the pressure given is
gauge.
% Therefore absolute pressure in tank is P1a=P1 + 101.325 = 104.325
kPa.
% Initial in tank at 1 velocity V1 = 0 m/s and P3 =Patm = 101.325
kPa.
% Also it is not mentioned about any head loss in the hose.
Considering it
% as ideal streamlined flow from tank to hose to outside through
nozzle.
% Applying Bernoulli's Equation between 1 and 2.
% P1a/Rho + V1^2/2 = P2a/Rho + V2^2/2 ..........(1)
% Applying continuity beteen 2 and 3 Q=flow rate
% Q2=Q3 .......................................(2)
% Applying Bernoulli's Equation between 2 and 3.
% P2a/Rho + V2^2/2 = P3/Rho + V3^2/2 ...........(3)
% From (1) and (3) :
% P1a/Rho + V1^2/2 = P3/Rho + V3^2/2 ...........(4)
%% Initializing the Problem
P1 = 3; % in kPa
Patm = 101.325; % in kPa
T = 273.15; % in Kelvin
P1a = 3 + Patm; % in kPa
V1 = 0; % in m/s
D = 0.02; % in m
d = 0.01; % in m
a3=pi*d^2/4; % Area of nozzle at exit in m^2
A2=pi*D^2/4; % Area of hose at exit in m^2
P3=Patm;
R = 0.287; % Gas constant for air in kJ/kgK;
Rho = Patm/(R*T); % in kg/m^3 for air.
%% Solving the problem
% From eqn(4)
V3=sqrt(2*1000*(P1a-P3)/Rho);
Q3 = V3*a3 % Flow rate in m^3/sec
% From eqn(2)
V2=Q3/A2;
% From eqn(3)
P2a = (-V2^2/2 + P3*1000/Rho + V3^2/2)*Rho/1000;
P2=P2a-Patm
Please comment below for any further queries
Thank you
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