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Simulating Crowd-induced vibrations using the Duhamel Integral

by Dr Seán Carroll
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Published: 25th January 2022
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Python Project

In this Python mini-project, you’ll learn about the Duhamel Integral and how it can be used to simulate the dynamic response of a single degree of freedom system. We’ll discuss how to solve the integral and then write some Python code to implement our solution for any arbitrary loading. In the second half of this project, we’re going to use our Duhamel Integral solver to build a crowd loading simulation. This will allow us to simulate the vibration response of a footbridge to pedestrian traffic. 

Duhamel Integral-small | DegreeTutors.com

Download the Complete Python Code for this Crowd-induced Vibration Simulator

As usual, this project is accompanied by a complete HD video series. You can access the full playlist directly below or by enrolling in the project on DegreeTutors.com (link above). In the video series, we’ll walk through the build process line by line. So you can build along with me or if you prefer, just download the finished Python code after you enrol in the project. I recommend reading through this post to get a good overview of the build process and then working through the tutorial videos in more detail.

Playlist

8 Videos
Play Video

If you’re new to Python, don’t worry – you don’t need to be a Python programmer to complete this project! Complete beginners can work through this project and pick up the programming basics along the way. If you need help getting your coding environment setup, check out this video (part of another course but covers what you need to get up and running). So, with all of that out of the way, let’s get into it.

1.0 The Duhamel Integral – Basic Concept

The Duhamel integral is a simple way to simulate the response of a single-degree-of-freedom (SDoF) system to any form of dynamic loading. When the loading is described by a simple mathematical function, we can analytically solve the integral. However, for practical application, this is very often not the case. If the loading is more complex or defined by a time-history of discrete force values, numerical integration can be employed.

We’ll cover the details of how the integration can be handled in both cases. For now, we just need to understand the concept behind the Duhamel integration approach. We can start by considering an impulse. This is simply a force, p(t), that is applied for a very short duration, say \delta t. The impulse of the force is defined as the area below the force-time history. So, a unit impulse would have an area of 1,

Duhamel - img1 | DegreeTutors.com
Figure 1. Impulse associated with the force p(t) applied for duration \delta t

Now, let’s think about applying an impulse to a SDoF system. We’ll see below that we can determine an expression for the resulting free vibration response of the system. Remember, the impulse is a very short duration, high magnitude load. So, it will induce a short duration driven response followed by a decaying (we’ll assume a damped system) free vibration response.

So, how do we use this new information to simulate the response of a SDoF system to general dynamic loading? The trick is to consider the general dynamic loading as a sequence of short duration impulses. Each impulse will induce a free-vibration response. To obtain the overall dynamic response, we simply superimpose the free vibration responses due to each impulse, Fig. 2.

Duhamel - img2 | DegreeTutors.com
Figure 2. General dynamic loading considered as a sequence of N impulses yielding N free-vibration responses that can be superimposed to obtain the response to the original dynamic loading.

Hopefully you can see that at a concept level, there’s not much complexity to the Duhamel integral. It’s a very simple but versatile tool. There is one limitation to be aware of. Because we rely on superposition to obtain the overall structural response we must assume the behaviour of the dynamic system is linear. If this is not the case, an alternative solution strategy should be sought, such as direct integration of the equation(s) of motion. We cover this in more detail in my Multi-Degree of Freedom Dynamics course.

1.1 Damped Impulse Response

Our next task is to determine an expression for the impulse response of our SDoF system. We start by considering Newton’s second law which states that the rate of change of velocity is directly proportional to the force that causes it, mathematically we have,

(1)   \begin{equation*}F(\tau) = m\frac{\mathrm{d}v}{\mathrm{d}\tau}\end{equation*}

Rearranging slightly, we have,

(2)   \begin{equation*}F(\tau)\mathrm{d}\tau = m \mathrm{d}v\end{equation*}

Notice that F(\tau)\mathrm{d}\tau is actually an impulse; recall from above that the impulse associated with force p(t) was the area below the force-time history, p(t)\delta t. We can see that the impulse F(\tau)\mathrm{d}\tau induces an instantaneous change in velocity, \mathrm{d}v. Also note that we’ve introduced the time variable \tau, distinct from t, to represent the time of application of a specific impulse. This will become clearer when we see both \tau and t in the same expression below.

The instantaneous change in velocity, \mathrm{d}v can equally be interpreted as an initial velocity, v_0 associated with the application of the impulse,

(3)   \begin{equation*}\mathrm{d}v = v_0 = \frac{F(\tau)\mathrm{d}\tau}{m}\end{equation*}

Now our problem reduces to determining the free vibration response of a SDoF system with non-zero initial velocity v_0 at time \tau. We can show that the damped free vibration response of a SDoF system is given by,

(4)   \begin{equation*}u(t) = e^{-\xi\omega_n t}\left[\frac{v_0 + u_0\xi\omega_n}{\omega_d}\sin(\omega_d t) + u_0\cos(\omega_d t)\right]\end{equation*}

where, \xi is the damping ratio, \omega_n is the angular natural frequency, \omega_d is the damped natural frequency and u_0 is the initial displacement. We cover the derivation of this equation in my Fundamentals of Structural Dynamics course.

Now, if we assume the impulse is applied at time \tau, let u_0=0 and let v_0 equal to the value in equation 3, we can obtain an expression for the incremental response, \mathrm{d}u(t) due to the impulse F(\tau)\mathrm{d}\tau applied at time \tau,

(5)   \begin{equation*}\mathrm{d}u(t) = e^{-\xi\omega_n(t-\tau)}\left[\frac{F(\tau)\mathrm{d}\tau}{m\omega_d}\sin\omega_d(t-\tau)\right]\end{equation*}

Note that we now have the quantity of time elapsed since the impulse was applied, denoted as t-\tau. This is why we introduced the time variable \tau originally. We’re not quite finished; remember that to get the total response of the system at time t, we need to sum up or superimpose the influence of all of the impulses applied, up to this point in time. We can do this by integrating both sides of equation 5,

(6)   \begin{equation*}\boxed{u(t) = \frac{1}{m\omega_d}\int_0^t F(\tau) e^{-\xi\omega_n(t-\tau)}\sin \omega_d (t-\tau)\mathrm{d}\tau}\end{equation*}

This expression is what we refer to as Duhamel’s integral – the next step is to solve it.

2.0 Analytical Solution

As we said at the outset, there are two approaches to solving the Duhamel integral (or any integration really), analytical solution and numerical solution. By far the most practically useful method is numerical solution. Most of the interesting problems, from an engineering perspective, require numerical solution. Although a numerical solution will always be an approximation, any error introduced usually pales into insignificance when compared against other uncertainties bakes into our modelling.

Numerical solution comes with the huge advantages of simplicity and versatility. I’ve always been more of a programmer than a mathematician so I may be biased. Having said all of this, we will demonstrate an analytical solution first for completeness; even then we’ll use Python to do the hard work.

Ramp Loading

Consider a load that increases linearly from zero to a magnitude of P_0 between t=0 and t=t_1. We can represent the loading with a simple mathematical expression,

(7)   \begin{equation*}p(t) = \frac{P_0 t}{t_1}\end{equation*}

The fact that the applied loading can be captured with such a simple expression is the first clue that we might be able to solve this analytically. Assigning some arbitrary values to P_0 and t we can generate a plot of the loading.

Duhamel - img3 | DegreeTutors.com

Next, we can insert our expression for the applied loading directly into the Duhamel integral expression.

(8)   \begin{equation*}u(t) = \frac{1}{m\omega_d}\int_0^t \frac{P_0 \tau}{t_1} e^{-\xi\omega_n(t-\tau)}\sin \omega_d (t-\tau)\mathrm{d}\tau\end{equation*}

In this case, we are only considering the response of the system during the application of the ramp load and not the free vibration that would follow. As such, damping will not have an appreciable influence on the response. We can therefore simplify the task by considering an undamped system. As a result, our expression reduces to,

(9)   \begin{equation*}u(t) = \frac{P_0}{t_1 m\omega_n}\int_0^t \tau \sin \omega_n (t-\tau)\mathrm{d}\tau\end{equation*}

Now we need to integrate this expression, for this we’ll use SymPy.

Combining the output from SymPy with the remaining elements from equation 9 yields,

(10)   \begin{equation*}u(t) = \frac{P_0}{t_1 m \omega_n}\left(\frac{t}{\omega_n}-\frac{\sin(\omega_n t)}{\omega_n^2}\right)\end{equation*}

We can further rearrange this,

(11)   \begin{equation*}u(t) = \frac{P_0}{k}\left[\frac{t}{t_1} - \frac{\sin(\omega_n t)}{\omega_n t_1}\right]\end{equation*}

To complete the picture, we can plot the response. When plotting we will normalise the time axis by the rise time t_1 and normalise the displacement axis by the maximum static displacement, P_0/k.

We’ll perform the response calculation for a range of different SDoF systems with the same mass but different stiffness, yielding a range of natural frequencies. For each system, we’ll specify the period of the system as a proportion of the rise time of the load.

Duhamel - img4 | DegreeTutors.com

This example is a relatively trivial case but it demonstrates the analytical integration route to solving the Duhamel integral. As I mentioned, you’re not likely to deploy analytical integration too often, so we’ll leave this method behind and focus on numerical integration from here on.

3.0 Numerical solution

From what we’ve seen so far, solving the Duhamel integral analytically is certainly possible, but as we’ve already mentioned, real-life engineering is messy and often we can’t neatly describe our applied loading in a mathematical function. This is where the numerical solution strategy comes in. In this section we’ll build a function that numerically solves the Duhamel integral for any arbitrary loading we pass into the function. We’ll start by restating the Duhamel integral for a damped system,

(12)   \begin{equation*}u(t) = \frac{1}{m\omega_d}\int_0^t F(\tau) e^{-\xi\omega_n(t-\tau)}\sin \omega_d (t-\tau)\mathrm{d}\tau\end{equation*}

We can separate out the time variables with the help of a trigonometric identity,

(13)   \begin{equation*}u(t) = \frac{1}{m\omega_d} e^{-\xi\omega_n t}\int_0^t F(\tau) e^{\xi\omega_n\tau} \left[ \sin (\omega_d t) \cos (\omega_d \tau) - \cos (\omega_d t) \sin (\omega_d \tau) \right] \mathrm{d}\tau\end{equation*}

Since we’re integrating with respect to \tau we can restructure our expression to isolate the terms requiring numerical integration,

(14)   \begin{equation*}u(t) = A e^{-\xi \omega_n t} \sin (\omega_d t) - Be^{-\xi\omega_n t} \cos(\omega_d t)\end{equation*}

where,

(15)   \begin{equation*}A = \frac{1}{m\omega_d} \int_0^t e^{\xi \omega_n \tau} F(\tau)\cos(\omega_d\tau)\mathrm{d}\tau\end{equation*}

(16)   \begin{equation*}B = \frac{1}{m\omega_d} \int_0^t e^{\xi \omega_n \tau} F(\tau)\sin(\omega_d\tau)\mathrm{d}\tau\end{equation*}

A and B now represent two integrals that we can numerically evaluate. We’ll use the trapezoidal rule here; we’ve covered this in some detail in our beam deflection calculator project so we’ll only briefly summarise the key points here.

If we consider the integrand (of A or B) as a simple function, f(\tau), we could plot this function on a \tau-f(\tau) plane. We know that the integration is simply the area bounded by the function and the horizontal axis. Using the trapezoidal rule we can approximate this as,

(17)   \begin{equation*}\text{Area} = \int_0^{t_n} f(\tau) \mathrm{d}\tau \approx \frac{\Delta_t}{2}\left[f(t_0) + 2f(t_1)+\ldots + 2f(t_{n-1}) + f(t_n)\right]\end{equation*}

Now all that remains is to write a function to cycle through the time history computing the numerical integrations in equations 15 and 16 and then compute the response using equation 14.

3.1 Implementing the numerical solution

We’ll package all of our code into a function that accepts a time and force vector. This way we can easily reuse the Duhamel integral function from this file and deploy it elsewhere down the road. Let’s start by defining SDoF system parameters; mass m, damping ratio \xi and natural frequency/angular natural frequency f_n/\omega_n. We can also define the damped natural frequency, \omega_d = \omega_n\sqrt{1-\xi^2}.

For the purposes of demonstration here we’ll define a harmonic forcing function. This will make it easier to validate our Duhamel integral function against a closed-form solution. First, we can define a time vector in the usual way.

The function we write next will accept the time and force vectors as arguments. We’ll rely on the fact that all of the system parameters a defined globally so we won’t bother explicitly passing them into the function. We basically need to cycle through the time record and compute the area of the i^{th} trapezoid and add this to a cumulative sum of areas as we move along the time axis. In this way, we can calculate appropriate values for A and B (equations 15 and 16) at each time-step. Then, we can calculate the actual response for each time-step using equation 14. If I’ve lost you with the trapezoidal method of numerical integration, go back to the beam deflection tutorial I referenced earlier. I walk through this technique from scratch there.

Now that we have the function defined we just need to call it and assign the output to a variable for plotting.

Duhamel - img5 | DegreeTutors.com

We can see above that the response contains a transient component that dissipates due to damping leaving a steady-state response which is exactly what we would expect from the harmonic excitation of a SDoF system.

4.0 Validating our numerical solution

Now we’ll confirm the validity of our Duhamel function by comparing the calculated response with the closed-form (analytical) solution for harmonic loading of a SDoF system. We could plot the complete closed-form response including the transient and steady-state components but for our validation exercise it will be sufficient to only plot the steady-state response, u_s(t) given by,

(18)   \begin{equation*}u_s(t) = \frac{P}{k}\left[ \frac{1}{(1-\beta^2)^2 + (2\xi\beta)^2} \right] \left[ (1-\beta^2)\sin(\omega t)-2\xi\beta\cos(\omega t) \right]\end{equation*}

If you’ve studied fundamental structural dynamics, you will recognise this as the dimensionless form of the steady-state response equation – if this is completely unfamiliar and you don’t like equations dropping out of thin air, go here.

Duhamel - img6 | DegreeTutors.com

We can see that both solutions agree once the transient response has decayed away. This gives us confidence in the Duhamel integral code we’ve written. This is quite a powerful tool we have at our disposal now. Although we only used it to calculate the response due to harmonic loading, we can feed it any forcing function and it will return the SDoF system response.

So, in the next phase of this project, we’ll use our Duhamel integral function to do something a little more interesting. We’re going to estimate the vertical vibration response of a footbridge to pedestrian traffic. Although, we’ll focus on a simply-supported footbridge, the same principles can be applied to crowd-induced vibration of any structure, although there are some specific caveats we’ll discuss along the way.

5.0 An introduction to dynamic crowd loading

Volumes of research has been produced on the topic of human-induced vibration and in particular crowd-induced vibration. Research in this area has intensified in the last 20 years as structures, in particular floor plates, have become lighter and more slender. This has resulted in unacceptably large occupant-induced vibrations being observed in service more frequently. There is now a much greater understanding among engineers and other procurement stakeholders about the need to carefully asses vibration serviceability at design stage.

For the purposes of this analysis project, when we say human-induced vibration, we’re referring to the vibration induced by a single pedestrian as they walk. Crowd-induced vibration will refer to the response induced by multiple people simultaneously walking across a structure.

Human-induced vibration is a complex and fascinating dynamic problem because it involves interaction between the structure and the occupying pedestrian, both of which are dynamic systems. The problem gets even more interesting (and complex) when we start to introduce interaction between pedestrians and try to capture the tendency for a pedestrian to be influenced by the behaviour of those around them. We won’t attempt to dive in to the detail too much here but we do need some understanding of the problem before we start coding.

In addition to dividing the problem into human-induced and crowd-induced vibration, we can further divide the problem into one that considers vertical vibration and one that considers lateral vibration. Human locomotion response and balance behaviour is very different in each case. We’ll focus here on vertical vibration and leave the juicy problem of lateral human-structure interaction and synchronisation for another day!

Footfall force modelling 101

In the simplest of terms, when a person walks across a structure, in our case a linear footbridge, they will apply a vertical footfall force or ground reaction force (GRF) with each footstep. We can crudely model this GRF using a sine function, or more specifically a series of sine functions representing the harmonic components of the GRF. This assumes that the GRF is perfectly periodic which is itself a simplification but we can live with it. So, the GRF can be represented as the static weight of the pedestrian, G, added to a Fourier series representing the dynamic component of loading,

(19)   \begin{equation*}F_v(t) = G + \sum_{i=1}^n G\:\text{DLF}_i\sin(2\pi i f_v t - \phi_i)\end{equation*}

where, \text{DLF}_i is the i^{th} Fourier coefficient (also knows as a Dynamic Load Factor), \phi_i is the phase of the i^{th} harmonic and f_v is the pacing frequency. We will only concern ourselves with the fundamental harmonic, i.e. that component of the GRF at the pacing frequency. We’ll ignore the higher integer harmonics in this example, but these may be significant, depending on the dynamic characteristics of the structure in question.

In order to model the GRF we need to know the Fourier coefficient of the fundamental harmonic. Again there has been a lot of research work on this over the years but we’ll use an early relationship proposed by Kerr [1] that relates the DLF to the pacing frequency, f_v,

(20)   \begin{equation*}\text{DLF} = 0.41(f_v-0.95) \leq 0.56\end{equation*}

This relationship is valid for pacing frequencies between 1\: Hz and 2.8 \:Hz. Now, this raises the question of what should the pacing frequency be? For this we’ll rely on a relationship presented by Bruno and Venuti [2] that was developed from the earlier work of Bertram & Ruinne [3],

(21)   \begin{equation*}f_v = 0.35v_p^3 -1.59v_p^2+2.93v_p\end{equation*}

where v_p is the walking velocity. Of course now we’re presented with the task of working out what a sensible walking velocity should be. Here we’ll rely on work by Pachi and Ji [4] who observed that walking velocities in a sample of pedestrians were normally distributed with a mean value of 1.3\:m/s and a standard deviation of 0.125\:m/s.

An import feature in the modelling of crowd-induced vibration is the flow behaviour of the pedestrian crowd and their evolving distribution across the structure. As a pedestrian crowd becomes more dense, walking velocities are reduced due to congestion. However in this analysis, we’ll ignore all traffic effects due to interaction between pedestrians. This is a reasonable assumption for uncongested crowds where it’s reasonable to expect that an individual’s desired walking velocity won’t be constrained by neighbouring pedestrians.

We’re now at a point where we can approximate the GRF imparted by a pedestrian with a mass of 80\:kg walking with a velocity of 1.3\:m/s in a straight line. If we assume the pedestrian walks across a 60\:m long footbridge, it will take then 60\:m/1.3\:m/s = 76.9 seconds to cross the bridge. This gives us the duration of load application.

Now we can define the time vector and plot the GRF. Note that we’re only interested in the positive value of the GRF as the footfall force never acts to pull the walking surface upwards! This means that a single sine wave actually models 2 footsteps – this is why the frequency is divided by 2 in the code below.

Duhamel - img7 | DegreeTutors.com

Each of the half-sine peaks represents the force generated by one foot hitting the surface. Remember, a more rigorous model would need to consider the influence of varying walking speed. Even when we make the assumption of constant walking speed, the GRF is not a perfectly periodic function so there is some approximation involved in representing it as a Fourier series.

Furthermore, we’re only representing the fundamental harmonic component here – an actual recorded GRF resembles a square wave more than a half-sine wave. Nevertheless, this will still give us a reasonably realistic first approximation of human-induced vibration response when we apply it to a structure.

It’s also worth pointing out that in our modelling we’re going to assume that there is no human-structure interaction. This is generally a bigger problem for lateral oscillations, due to the fact that humans tend to exhibit higher sensitivity to lateral support motion versus vertical motion. This is likely a result of our bi-pedal nature and inherent instability in the lateral direction. So, just to be clear, we’re assuming the vertical bridge motion does not influence the pedestrians behaviour (and their GRF) in any way.

The bridge/beam structure

Now we can turn our attention to the bridge structure. We’ll keep things simple here and assume that our bridge can be modelled as a simply supported beam. This means that the modal properties are easily obtained. In particular we’re interested in the mode shapes, \phi_n(x) which can be obtained from,

(22)   \begin{equation*}\phi_n(x) = \sin \frac{n\pi x}{L}\end{equation*}

where n is the mode number and x is the longitudinal coordinate along the bridge/beam. For a deeper dive into modal analysis, refer to my Multi-Degree of Freedom Dynamics course. We’re going to assume that the fundamental vertical mode of the bridge has a frequency of 2.5\:Hz. This is sufficiently close to the average pacing frequency that if this were a real bridge we would be concerned that unacceptable vibrations may be observed in service.

We’ll assume that the bridge has a damping ratio of 2.5\:\% and that the mass per unit length, M is 2000\:kg/m. We’re going to make another simplifying assumption here; we’ll assume that the mass of pedestrians on the bridge has no influence on the modal mass of the dynamic system being simulated. Our justification here is that the mass of pedestrians is insignificant compared to the mass of the bridge. If this were not the case we could consider modifying the modal mass to reflect the evolving distribution of pedestrians on the bridge. I published a paper [5] on this some time ago that you can read if you want to explore this further. Thanks to this simplification, the modal mass, m_n remains constant and can be calculated from the expression,

(23)   \begin{align*}m_n &= M\int_0^L \phi_n(x)^2 \mathrm{d}x \\&= M\int_0^L \sin^2\frac{\pi x}{L} \mathrm{d}x \\&= \frac{ML}{2}\end{align*}

So, for the first mode, the modal mass is simply half the actual mass of the structure.

6.0 Dynamic analysis: Bridge + 1 pedestrian

Since we’re assuming that the bridge has only one modal frequency in the range of interest, we only need to simulate a single vibration mode which makes the Duhamel integral an ideal solution technique. Conveniently for us and through the magic of modal analysis, this means that the dynamic analysis of the bridge reduces to simulating the response of a SDoF system. If we needed to simulate the combined response of multiple modes, this is easily done through modal superposition.

Our first task is to turn our GRF, F_v, into a modal force, F_n. This simply means multiplying it by the unity-normalised mode shape value at the pedestrian’s location, x_p,

(24)   \begin{equation*}F_n = F_v\phi (x_p)\end{equation*}

Since our pedestrian is walking with a constant velocity, we can easily determine their position, x_p, as a function of time. From here we can determine the value of the mode shape as a function of time and directly multiply this by the GRF calculated earlier to obtain the modal load applied to the SDoF modal model as a function of time.

At this point it’s helpful to visualise the modal force. Remember, this is the force applied to the first bridge/beam mode with a half-sine mode shape. We can think of this force as the influence of the GRF on mode one which is at a maximum at the centre-span position.

Duhamel - img8 | DegreeTutors.com

We can clearly see that the dynamic influence of the pedestrian’s GRF is increasing as they move towards the centre of the bridge and diminishing thereafter. Now it’s just a matter of providing this force along with the time vector directly into our Duhamel function. Since our function relies on globally defined variables, we need to be careful to redefine these for our bridge before calling the function.

Duhamel - img9 | DegreeTutors.com

After plotting the modal response we can see the oscillation behaviour superimposed on top of the static deflection. We can visualise this more clearly if we separate out the static and dynamic components of the GRF and simulate their influence separately.

Duhamel - img10 | DegreeTutors.com

It will help us to more clearly visualise the response if we write a quick function to plot the displacement envelope. This will be particularly helpful later on when our response is derived from the influence of many pedestrians walking simultaneously. We’ll do this by cycling through the displacement record and extracting the oscillation peaks. A peak will be identified when the slope of the displacement changes sign from positive to negative.

This won’t be a perfect strategy as it will also identify ‘minor’ peaks due to frequencies other than the dominant oscillation frequency but it will be close enough for visualisation purposes. Again, we’ll package the code into a function that can be easily called multiple times.

Now we can plot the response again but also plot an envelope line that spans between oscillation peaks.

Duhamel - img11 | DegreeTutors.com

Follow the final two parts of this project over on DegreeTutors:Labs

Now that we can simulate the mid-span response induced by a single pedestrian as they cross the bridge, we’re ready to expand our simulation to consider a pedestrian crowd consisting of N pedestrians. To follow the final two parts of this project,

continue reading (for free) over on our content hub, DegreeTutors:Labs where each section of this project is broken out into individual lectures. 

I hope you’ve enjoyed what you’ve read so far and finish the project over on DegreeTutors:Labs. Remember that you can download all of the code for this project by following the link at the top of this tutorial. If you want to take a deeper dive into structural dynamics, check out the Structural Dynamics course bundle below. This will give you a clear roadmap to mastering structural dynamics and implementing what you know with Python.

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Dr Seán Carroll

BEng (Hons), MSc, PhD, CEng MIEI, FHEA

Hi, I’m Seán, the founder of DegreeTutors.com. I hope you found this tutorial helpful. After spending 10 years as a university lecturer in structural engineering, I started DegreeTutors.com to help more people understand engineering and get as much enjoyment from studying it as I do. Feel free to get in touch or follow DegreeTutors on any of the social accounts.

References
[1] S.C. Kerr, Human Induced Loading on Staircases, Ph.D. Thesis, University College London, Mechanical Engineering Department, London, UK, 1998.
[2] F. Bruno, L.and Venuti. Crowd-structure interaction in footbridges: Modelling, application to a real case-study and sensitivity analyses. Journal of Sound and Vibration, 323:475–493, 2009.
[3] J. E. A. Bertram and A. Ruina. Multiple walking speed-frequency relations are predicted by constrained optimization. Journal of Theoretical Biology, 209:445–453, 2001.
[4] A. Pachi and T. Ji. Frequency and velocity of people walking. The Structural Engineer, 83:36–40, 2005.
[5] S.P. Carroll, J.S. Owen, M.F.M. Hussein. Modelling crowd-bridge dynamic interaction with a discretely defined crowd. The Journal of Sound and Vibration, 331:2685-2709, 2012

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